Isolation of bacteriophage MX4, a generalized transducing phage for Myxococcus xanthus.

The structure of α-chitin has been determined by X-ray diffraction, based on the intensity data from deproteinized lobster tendon. Least-squares refinement shows that adjacent chains have alternating sense (i.e. are antiparallel). In addition, there is a statistical distribution of side-chain orientations, such that all the hydroxyl groups form hydrogen bonds. The unit cell is orthorhombic with dimensions a = 0.474 ± 0.001 nm, b = 1.886 ± 0.002 nm and c = 1.032 ± 0.002 nm (fiber axis); the space group is P2₁2₁2₁ and the cell contains disaccharide sections of the two chains passing through the center and corner of the ab projection. The chains form hydrogen-bonded sheets linked by CO…HN bonds approximately parallel to the a axis, and each chain has an O-3′H…O.5 intramolecular hydrogen bond, similar to that in cellulose. Adjacent chains along the ab diagonal have different conformations for the CH₂OH groups: on one chain these groups form O.6H…O.6′ intermolecular hydrogen bonds to the CH₂OH group on the adjacent chain along the ab diagonal. The latter group is oriented to form an intramolecular O.6′H…O.7 bond to the carboxyl oxygen on the next residue. The results indicate that a statistical mixture of CH₂OH orientations is present, equivalent to half oxygens on each residue, each forming inter- and intramolecular hydrogen bonds. As a result the structure contains two types of amide groups, which differ in their hydrogen bonding, and account for the splitting of the amide I band in the infrared spectrum. The Inability of this chitin polymorph to swell on soaking in water is explained by the extensive intermolecular hydrogen bonding.     

The crystal and molecular structure of tri-o-ethylamylose (tea 3)

The crystal and molecular structure of a tri-O-ethylamylose polymorph, TEA 3, has been solved by stereochemical conformation and packing analysis, combined with X-ray fibre diffraction analysis. The unit cell is orthorhombic, space group P2₁2₁2₁, with a  15.36 (±0.03) Å, b  12.18 (±0.05) Å, and c (fibre repeat)  15.48 (±0.01) Å. The actual chain conformation is a 4₃ helix with the EtO-6 group in the tg position, as was found in the polymorph TEA 1.     

The crystal structure of d-glucose 6-(sodium hydrogen-phosphate)

The title compound, when recrystallised from water, is monoclinic, space group P2₁, with a = 5.774(4), b = 7.189(5), c = 12.69(1) Å, β = 106.66(5)°, and Z = 2. The crystal structure was determined from three-dimensional X-ray diffraction data taken on an automatic diffractometer with CuKα, and refined by least-squares techniques to R = 0.034 for 977 reflexions. The pyranose ring adopts the ⁴C₁ conformation. The conformation about the exocyclic C-5-C-6 bond is gauche-trans [the torsion angles O-6-C-6-C-5-O-5 and O-6-C-6-C-5-C-4 are 64.2(8) and ?175.6(7)°, respectively], which is significantly different from the gauche-gauche geometry in d-glucose 6-(barium phosphate). The phosphate ester bond, P-O-6, is 1.584(3) Å. All of the oxygen-bonded hydrogen atoms are involved in intermolecular hydrogen-bonds.     

Crystal structure of zinc citrate

The crystal structure of zinc citrate [Zn(II) (C₆H₅O₇)₂·4NH₄⁺] shows isolated zinc ions octahedrally coordinated to two equivalent citrates via a central hydroxyl, central carboxyl, and one terminal carboxyl from each citrate. The clusters are linked through hydrogen bonds to ammonium ions in the lattice. The structure is distinctly different from that of other divalent cation triply ionized citrate complexes, which are polymeric. Crystal data : space group P2₁/C, a = 8.784(3) Å, b = 13.499(4) Å, c = 9.083(3) Å, β = 113.4°(1), V = 988(1) ų. Citrate has been identified as the low molecular weight ligand that complexes zinc in human milk; this may be of interest in relation to intestinal zinc absorption.     

f-Element/crown ether complexes. 1. Synthesis and structure of [Y(OH2)8]Cl3·(15-crown-5)

The crystal and molecular structure of [Y(OH₂)₈]Cl₃·(15-crown-5) has been determined by single- crystal X-ray diffraction. The complex crystallizes in the monoclinic space group P2₁/n with Z = 4. Lattice parameters are a = 9.202(2), b = 17.247(3), c = 15.208(3) Å, and β = 92.39(2)°. The structure was solved by Patterson and Fourier techniques and refined by least-squares to a final conventional R value of 0.081. The Y(III) ion is eight coordinate, bonded to the oxygen atoms of the eight water molecules. Three of the water molecules are hydrogen bonded to crown ether molecules. The three chloride ions participate in hydrogen bonds with the remaining five water molecules. The YO(water) distances range from 2.322(6) to 2.432(7) Å and average 2.37(4) Å. The average O(water)···Cl and O(water)···O(crown) hydrogen bonded separations are 3.08(4) and 2.76(7) Å, respectively.     

f-element/crown ether complexes. 6. Interaction of hydrated lanthanide chlorides with 15-crown-5: Crystallization and structures of [M(OH2)8]Cl3·(15-crown-5) (M = Gd,Lu)

The interaction of hydrated chloride salts of Gd³⁺ and Lu³⁺ with 15-crown-5 in a 1:3 mixture of CH₃OH:CH₃CN produces crystalline [M(OH₂)₈]Cl₃· (15-crown-5) (M = Gd, Lu). The crystal and molecular structures of both complexes have been determined by single crystal X-ray diffraction. Both are isostructural with previously determined Y analog and crystallize in the monoclinic space group P2₁/n with Z = 4. Lattice parameters are a = 9.247(4), b = 17.312(5), c = 15.191(6) Å, β = 92.19(3)°, D_calc = 1.72 g cm⁻³ for M = Gd and a = 9.150(1), b = 17.171(1), c = 15.217(1) Å, β = 92.64(1)°, D_calc = 1.80 g cm⁻³ for M = Lu. Each complex was refined by least-squares to final conventional R values of 0.052 (M = Gd, 2932 observed [F_o⩾5σ(F_o) reflections) and 0.036 (M = Lu, 3313 observed reflections). The octaaquo M(III) ions exist as a distorted dodecahedron with average MOH₂ separations of 2.41(4) Å (M = Gd) and 2.35(4) Å (M = Lu). The crown ether molecule is hydrogen bonded to metal coordinated water molecules to form polymeric chains along b. The remaining water molecule hydrogen atoms participate in hydrogen bonds with the chloride ions essentially in the ac plane. Two resolvable disordered crown ether conformations are observed with occupancies of 60%/40% (M = Gd) and 75%/25% (M = Lu).     

Molecular and crystal structure of the regenerated form of (1→3)-α-d-glucan

The crystal structure of a regenerated form of (1→3)-α-d-glucan, obtained by solid state deacetylation of the triacetate derivative, has been determined by combined X-ray diffraction analysis and stereochemical model refinement. The structure crystallizes in an orthorhombic unit cell with parameters $\text{a = 16.46}\text{A}\text{?}\text{, b = 9.55}\text{A}\text{?}$ and c (fibre repeat)=8.44 Å, and space group P2₁2₁2₁. The chain conformation is nearly completely extended and is very close to a 2/1 helix, even though the dimer residue is the crystallographic repeat unit. An intramolecular O(2)  O(4)′ hydrogen bond stabilizes the conformation and extensive intermolecular hydrogen-bonding abilizes the packing. The resulting structure is sheet-like, with an alternating polarity of chain directions within the sheet. In its sheet-like character, extensive hydrogen-bonding, and insolubility in water, this polymorph of (1→3)-α-d-glucan resembles regenerated cellulose. The reliability of the structure analysis is indicated by the X-ray residual R=0.206.     

A Gene Located at 56F1-2 inDrosophila melanogasterEncodes a Novel Metazoan β-like Subunit of Casein Kinase II

Drosophila melanogastercasein kinase II (DmCKII) is composed of catalytic α and regulatory β subunits associated as an α₂β₂heterotetramer. Using the two-hybrid system, we have screened aDrosophilaembryo cDNA library for proteins that interact with DmCKII α. One of the cDNAs encodes a novel β-like polypeptide, which we designate β′.In situhybridization localizes the corresponding gene to 56F1-2, a site distinct from that of both the β gene and theStellatefamily of β-like sequences. The predicted sequence of β′ is more closely related to the β subunit ofDrosophilaand other metazoans than to the Stellate family of proteins, suggesting that it is a second regulatory subunit.In vitroreconstitution studies show that a GST-β′ fusion protein associates with the α subunit to generate a tetrameric complex with regulatory properties similar to those of the native α₂β₂holoenzyme. The data are consistent with the proposed role of the β′ subunit as an integral component of the holoenzyme.     

Coral acid rich protein selects vaterite polymorph in vitro

Corals and other biomineralizing organisms use proteins and other molecules to form different crystalline polymorphs and biomineral structures. In corals, it’s been suggested that proteins such as Coral Acid Rich Proteins (CARPs) play a major role in the polymorph selection of their calcium carbonate (CaCO₃) aragonite exoskeleton. To date, four CARPs (1–4) have been characterized: each with a different amino acid composition and different temporal and spatial expression patterns during coral developmental stages. Interestingly, CARP3 is able to alter crystallization pathways in vitro, yet its function in this process remains enigmatic. To better understand the CARP3 function, we performed two independent in vitro CaCO₃ polymorph selection experiments using purified recombinant CARP3 at different concentrations and at low or zero Mg²⁺ concentration. Our results show that, in the absence of Mg²⁺, CARP3 selects for the vaterite polymorph and inhibits calcite. However, in the presence of a low concentration of Mg²⁺ and CARP3 both Mg-calcite and vaterite are formed, with the relative amount of Mg-calcite increasing with CARP3 concentration. In all conditions, CARP3 did not select for the aragonite polymorph, which is the polymorph associated to CARP3 in vivo, even in the presence of Mg²⁺ (Mg:Ca molar ratio equal to 1). These results further emphasize the importance of Mg:Ca molar ratios similar to that in seawater (Mg:Ca equal to 5) and the activity of the biological system in a aragonite polymorph selection in coral skeleton formation.     

Experimental conformational study of two peptides containing α-aminoisobutyric acid. Crystal structure of N-acetyl-α-aminoisobutyric acid methylamide

Some theoretical studies have predicted that the conformational freedom of the α-aminoisobutyric acid (H-Aib-OH) residue is restricted to the α-helical region of the Ramachandran map. In order to obtain conformational experimental data, two model peptide derivatives, MeCO-Aib-NHMe 1 and Bu^tCO-LPro-Aib-NHMe 2 , have been investigated. The Aib dipeptide 1 crystallizes in the monoclinic system (a = 12.71 Å, b = 10.19 Å, c = 7.29 Å, β = 110.02°, Cc space group) and its crystal structure was elucidated by x-ray diffraction analysis. The azimuthal angles depicting the molecular conformation (? = ?55.5°, ψ = ?39.3°) fall in the α-helical region of the Ramachandran map and molecules are hydrogen-bonded in a three-dimensional network. In CCl₄ solution, ir spectroscopy provides evidence for the occurrence of the so-called ₅ and C₇ conformers stabilized by the intramolecular i → i and i + 2 → i hydrogen bonds, respectively. The tripeptide 2 was studied in various solvents [CCl₄, CD₂Cl₂, CDCl₃, (CD₃)₂SO, and D₂O] by ir and pmr spectroscopies. It was shown to accommodate predominantly the βII folded state stabilized by the i + 3 → i hydrogen bond. All these experimental findings indicate that the Aib residue displays the same conformational behavior as the other natural chiral amino acid residues.     

A linear function for the melting behavior of lipids

The melting behavior of a variety of saturated long chain compounds is shown to be related to hydrocarbon chain length by the equation TN = C₀ + T_∞N where T is the absolute melting temperature, and N is the number of long chain carbon atoms. The constants C₀ and T_∞ are determined graphically or analytically from TN vs. N data. The linear relationship, derived from fundamental thermodynamic principles, is empirically satisfied. For each homologous series considered, coefficients of the equation provide a rational means for correlation and comparison with other polymorphs and indicate the relative importance of chain length, chain parity (even or odd), and headgroup polarity to melting behavior.     

Metal ions-nucleobases interactions: preparation and crystal structures of trichloroadeninium zinc(ii)(form ii) and a similar zinc complex of arprinocid [6-amino-9-(2-chloro-6-fluorobenzyl)purine]

Two zinc complexes—trichloroadeninium zinc(II)(Form 11), C₅H₆N₅Cl₃Zn [structure(I)] and a similar complex of Arprinocid, (6-amino-9-(2-chloro-6-fluorobenzyl)purine], C₁₂H₁₀N₅FCl₄Zn [structure(II)]—have been prepared Structure(I) crystallizes in the space group P2₁/c with a = 8.223(1)Å, b = 6.755(1) Å, c = 18.698(3) Å, β = 96.10(2)°,and Z = 4. Structure(II) crystallizes in the space group P2₁/c with a = 8.209(2) Å, b = 6.421(8) Å, c = 31.794(8) Å, β = 90.76(2)°, and Z = 4. Both of these structures were solved by the heavy atom method using diffractometric data and refined to R = 0.028 [structure(I)] and 0.038 [structure(II)]. Zinc with a distorted tetrahedral coordination having three chlorines and N(7) as ligators, protonation of the adenine moiety at N(1), dissymmetry of exocyclic angles at N(7), and an interligand hydrogen bond (“indirect chelation”) involving one of the three chlorines, coordinated to zinc and a proton of the exocylic amino group are the striking features common to both structures. Similar types of indirect chelation as observed in the different complexes of purines have been discussed. The zinc ion deviates from the imidazole plane by 0.412 Å in structure(I) and 0.524 Å in Structure(II). The imidazol and pyrimidine planes fold about the C(4)-C(5) bond by 2.4° in strctur(I) and 3.8° in structure(II). In structure(I), inversion related molecules are paired through N(9)-H…N(3) hydrogen bonds. N-H…Cl hydrogen bonds and C(8)-H…Cl interactions have been observed in both structures.     

Beta structure of periodic copolypeptides of L-alanine and glycine. Their relevance to the structure of silks

The β structure of seven periodic copolypeptides of l-alanine and glycine² namely: A₂G, AG, A₂G₂, A₃G₃, A₂G₃, AG₂ and AG₃ has been studied by infrared, X-ray and electron diffraction techniques. The sheets are made of anti-parallel chains and intersheet spacing is observed to depend both on residue sequence and composition. Samples with glycine molar fractions varying from 0.33 to 0.6 are found to be good models for group II of silk fibroins. The structure of Bombyx mori silk fibroin is discussed in the light of these new data.     

The two beta forms of poly(L-glutamic acid).

β-Helical poly(L -glutamic acid) in a gel state was found to be easily converted to the antiparallel β form by heating. Two β forms were obtained, depending on the temperature of heating. Temperatures between 40° and 85°C produced a β form with a spacing between pleated sheets (d₀₀₁) of 9.03 Å, termed β₁. If the heating was carried out at temperatures higher than 85°C, the β₁ form underwent another conformational transition reducing the d₀₀₁ value from 9.03 to 7.83 Å (termed β₂) without any prominent change in the fiber repeat distance (i.e., the polypeptide backbone conformation). The time course of these two transitions was followed by measuring the infrared spectra of the samples, and it was concluded that the α → β₁ transition in its initial stage obeys a pseudo-first order rate process with activation enthalpy and entropy of 54 kcal/mol and 92 eu, respectively. On the other hand, the typical sigmoidal conversion curves observed for the transition between the two types of β forms (β₁ → β₂) indicate that this transition proceeds via a socalled “nucleation and growth” process. The kinetic theory of phase transitions developed by Avrami can be applied with success to explain this transition. The infrared spectra, in the region from 1800 to 200 cm^?1, were measured for these two β forms and the results showed that the conformation of the side chains and the mode of the hydrogen bonding between the side-chain carboxyl groups undergo appreciable change during the transition. The heat-induced conformational transition of poly(L -Glu⁷⁸ L -Val²²) was also studied. The copolymer was transformed from the α-helical conformation directly to the β₂ form. The reason for this was thought to be due to the fact that the L -valine residues and the L -glutamyl residues near the L -valine residues have a strong tendency to take the more compact β₂ form.     

f-Element/crown ether complexes. 26. Crystallization of two hydrated forms of hydrogen bonded complexes of NdCl3·nH2O and 15-crown-5. Crystal structures of [Nd(OH2)9]Cl3·15-crown-5·H2O and [NdCl2(OH2)6]Cl·15-crown-5

When slowly evaporated, the reaction of NdCl₃· nH₂O with 15-crown-5 in a 3:1 mixture of acetonitrile:methanol produces two crystalline hydrates. The decahydrate, [Nd(OH₂)₉]Cl₃·15-crown-5·H₂O, is orthorhombic, P2₁2₁2₁, with (at −150 °C) a = 10.571(4), b = 15.220(7), c = 15.686(7) Å, and D_calc = 1.71 g cm⁻³ for Z = 4. These crystals are stable to the moisture in air. Each Nd is nine-coordinate with tricapped trigonal prismatic geometry. The nine coordinated water molecules are hydrogen bonded to two symmetry related crown ethers, all three chloride ions, and the tenth water molecule. The crown has a total of six hydrogen bonds, four on one side (two to a single oxygen atom) and two on the other. This ether exhibits conformational disorder. The hexahydrate, [NdCl₂(OH₂)₆]Cl·15-crown-5 is deliquescent, dissolving in air and recrystallizing as [NdCl₂(OH₂)₆]Cl. Crystals of this complex are monoclinic, P2₁/n, with (at 20 °C) a = 9.821(3), b = 16.978(9), c = 12.849(8) Å, β = 94.06(5)°, and D_calc = 1.80 g cm⁻³ for Z = 4. The Nd atom exists in a distorted dodecahedral geometry with one chlorine in an A site and one in a B site. The coordinated chlorine atoms accept hydrogen bonds producing polymeric zigzag hydrogen bonded chains along c. The third noncoordinated chloride ion accepts four hydrogen bonds, three from one formula unit and one from a second formula unit related by a unit translation along a. The crown ethers accept five hydrogen bonds, two on one side, and three on the other, thus separating the zigzag chains along b.     

Polymorphism in [(polyamine)Co(NO2)x]Y crystals caused by changes in torsional angles of the (amine)N-Co-N-O fragments (x = 2, Y = NO3: x = 3, Y = 0)

Herein, we report the synthesis and characterization of a third polymorph of trans-[Co(2,3,2-tet)(NO₂)₂]NO₃, III, crystallizing in space group (No. 2) obtained during an attempt to reproduce the synthesis of a previously reported polymorph, I (for more details of polymorphs I and II, see Introduction and references cited therein). The cations of polymorphs I and II differ primarily by the angles that the planes of the two -NO₂ ligands make with one another; the former being considerably larger than that in II. Polymorph III resembles II in that the torsional angular differences between the trans-nitro ligands are also small, but differ notably from that in I.The structure of the compound [(5-Me-(dpt)Co(NO₂)₃], was determined also. The space group is P2₁/n, with two molecules in the asymmetric unit, whose occupancies are 65% and 35% for molecules IVa and IVb, respectively. Again, the two differ by the torsional angles of the nitro ligands, specially two of them whose angular orientations are vastly different. Molecules IVa and IVb are compared with a previously obtained polymorph V of this same compound reported earlier. Once more, V is closely related in stereochemistry to IVb, but differs markedly from IVa in nitro torsional angles.In all cases, the Co(amine) fragments are closely super-imposable and the differences in nitro torsional angles are the result of the availability of several amine hydrogens of the basal plane with which to make intra-molecular hydrogen bonds. Clearly, these hydrogen bonds must be of very similar strength and the barriers to rotation of the -NO₂ ligands must have energies similar to the energetics of the hydrogen bonds causing the torsional motions.     

Electron diffraction determination of chain packing of a ketonic insect wax

Single crystal electron diffraction patterns are obtained from thin microcrystals of two polymorphic forms of a pure ketonic wax secreted by the wooly alder aphid, Prociphilus tessellatus. One crystalline form gives intensity data which agree well with the commonly observed O_⊥ methylene subcell. The unit cell constants for the projection are $\text{a = 7.52}\text{A}\text{?}$ and $\text{b = 5.05}\text{A}\text{?}$. The other polymorph, which is found less often, is a rectangular supercell with pseudohexagonal symmetry in the intensity-weighted hk0 reciprocal net. The supercell parameters in projection are $\text{a = 42.06}\text{A}\text{?}$, and $\text{b = 9.12}\text{A}\text{?}$ with the inner order hexad of intense spots occurring at 4.20 Å.     

Hydrogen ion changes of rhodopsin I. Proton uptake during the metarhodopsin I 478 metarhodopsin II 308 reaction

The hydrogen ion changes resulting from the photolysis of the rod visual pigment, rhodopsin, have been investigated. Low temperature was used to isolate the metarhodopsin I₄₇₈ to II₃₈₀ reaction of rhodopsin and indicator dye was used to simultaneously measure the hydrogen ion changes of the rhodopsin solution.The results indicate that illuminated rhodopsin takes up a proton during the metarhodopsin I₄₇₈ to II₃₈₀ reaction and releases protons at later intermediate stages. The results are consistent with data indicating pK changes of rhodopsin as the basis for the R₂ phase of the early receptor potential and hydrogen ion changes of the medium or pK changes of rhodopsin as having effects on the late receptor potential.     

Significance of otolith calcium carbonate crystal structure diversity to microchemistry studies

Otoliths, calcium carbonate (CaCO₃) ear stones of fish, contain a wealth of information about fish life and environmental history yet the CaCO₃ polymorph form the otolith is made of is a critical, but seldom considered, piece of information during otolith analysis. Otolith trace element chemistry data increasingly informs management decisions, but recent work has shown that CaCO₃ polymorphs—aragonite, vaterite, and calcite—can bear on incorporation of trace elements in a non-trivial way. Most fishes are thought to have otoliths of the aragonite CaCO₃ form, but this construct is potentially outdated with many recent literature reports showing otherwise. Our study used previously unpublished neutron diffraction data and reports from published literature to address three objectives: (1) summarize the relative effects of otolith CaCO₃ polymorphism on otolith microchemistry, (2) summarize reports of otolith polymorphs to gain a better understanding of the extent of non-aragonite otoliths among fishes, (3) outline future research needed to align interpretations of microchemistry with our current understanding of otolith polymorph diversity. We found that while aragonite otoliths are the most common, so are exceptions. For example, the ostensibly rare (among species) CaCO₃ form vaterite was reported in at least some otoliths of 40% of the species surveyed. Our work suggests that examination of the CaCO₃ polymorph composition of otoliths should become more common particularly in studies where results will or may be used to inform management decisions. Future research should work to attribute controls on otolith CaCO₃ polymorph expression using a combination of -omics and material characterization approaches to enrich the life history and environmental information output from otoliths and increase our understanding of the assumptions made in otolith trace element chemistry studies.