Dirubidium dicadmium sulfate at 293 K

The structure of Rb₂Cd₂(SO₄)₃ at room temperature has been refined using X‐ray diffraction data. The structure is similar to that of other cubic langbeinites. However, the title compound differs from other type I langbeinites in that the bond‐valence sums of the metal cations (in particular the Rb atoms) are practically equal to their nominal chemical valences.     

1,3,5‐Triiodo‐2,4,6‐trimethylbenzene at 293 K

In the structure of tri­iodo­mesityl­ene (1,3,5‐tri­iodo‐2,4,6‐tri­methyl­benzene), C₉H₉I₃, at 293 K, the benzene ring is found to be significantly distorted from ideal D_6h symmetry; the average endocyclic angles facing the I atoms and the methyl groups are 123.8 (3) and 116.2 (3)°, respectively. The angle between the normal to the molecular plane and the normal to the (100) plane is 5.1°. No disorder was detected at 293 K. The thermal motion was investigated by a rigid‐body motion tensor analysis. Intra‐ and intermolecular contacts are described and topological differences compared with the isomorphous compounds tri­chloro­mesityl­ene and tri­bromo­mesityl­ene are discussed.     

4,4′‐Di­bromo­benzo­phenone at 293 and 103 K

The structure of 4,4′‐di­bromo­benzo­phenone, C₁₃H₈Br₂O, was determined at two different temperatures (293 and 103 K). A phase transition was not detected in this temperature range. Its crystal structure was found to be isostructural with that of the di­iodo analogue, but not with the structure of the di­chloro derivative.     

A urea complex of copper(II) hypophosphite at 293, 100 and 15 K

The crystal structure of poly­[copper(II)‐di‐μ‐hypophosphito‐μ‐urea], [Cu(H₂PO₂)₂(CH₄N₂O)]_n, has been determined at 293, 100 and 15 K. The geometry of the hypophosphite anion is very close to ideal, with point symmetry mm2. Each Cu atom lies on an inversion centre and is coordinated to six O atoms from four hypophosphite anions and two urea mol­ecules, forming a tetragonal bipyramid. The unique urea molecule lies on a twofold axis. Each hypophosphite anion in the structure is coordinated to two Cu atoms. The hypophosphite anions, urea mol­ecules and Cu^II cations form polymeric ribbons. The Cu^II cations in the ribbon are linked together by two hypophos­phite anions and a urea mol­ecule, which is coordinated to Cu via an O atom. The ribbons are linked to each other by N—­H?O hydrogen bonds and form polymeric layers.     

Na3Co(NO2)6 at 293 and 10 K

The crystal structure of trisodium hexanitro­cobaltate(III) has been determined by X‐ray diffraction at 293 and 10 K. It contains the slightly distorted octahedral Co(NO₂)₆^3? anion.     

Rinneite,K3Na[FeCl6], at 293, 84 and 9.5 K

The crystal structure of tripotassium sodium hexa­chloro­ferrate(II) has been determined by X‐ray diffraction at 293, 84 and 9.5 K. The accurate and extensive data sets collected should be suitable for charge–density analysis studies.     

A second monoclinic polymorph of S‐­(4‐tolyl) 4‐toluenethiosulfonate at 150 and 293 K

The title compound, C₁₄H₁₄O₂S₂, contains discrete mol­ecules and is a polymorph of a structure reported previously by Caputo, Palumbo, Nardelli & Pelizzi [Gazz. Chim. Ital. (1984), 114 , 421–430]. The present structure contains no intermolecular C—H?O hydrogen bonds, whereas in the previous polymorph, the mol­ecules are linked into continuous chains by such interactions.     

Cs2K[Mn(CN)6] at 293, 85 and 10 K

The crystal structure of dicaesium potassium hexacyanomanganese(III) has been determined by X‐ray diffraction at 293, 85 and 10 K. The Mn and K atoms lie on inversion centres and the Cs atom is in a general position. The accurate and extensive data sets collected should be suitable for charge–density analysis studies.     

Zwitterionic pyrrolidine‐2,2‐diylbis(phosphonic acid) at 100, 150 and 293 K

The title compound, C₄H₁₁NO₆P₂, reveals a two‐dimensional network of P—O—H?O=P and N—H?O=P hydrogen‐bond interactions, forming molecular slabs parallel with the (010) plane. One O—H?O interaction is distinct within these sets: whilst forming the shortest intermolecular hydrogen bond, it possesses a short P—O(H) bond of 1.5291 (10) Å. Weak C—H?O contacts link individual stacks to produce a three‐dimensional array. The compound is zwitterionic: one H atom from a P—O—H group has transferred to the pyrrolidine ring N atom.     

N‐Acetyl‐l‐tyrosine methyl ester monohydrate at 293 and 123 K

The crystal structure of a protected l ‐tyrosine, namely N‐acetyl‐l ‐tyrosine methyl ester monohydrate, C₁₂H₁₅NO₄·H₂O, was determined at both 293 (2) and 123 (2) K. The structure exhibits a network of O—H...O and N—H...O hydrogen bonds, in which the water molecule plays a crucial role as an acceptor of one and a donor of two hydrogen bonds. Molecules of water and of the protected l ‐tyrosine form hydrogen‐bonded layers perpendicular to [001]. C—H...π interactions are observed in the hydrophobic regions of the structure. The structure is similar to that of N‐acetyl‐l ‐tyrosine ethyl ester monohydrate [Soriano‐García (1993). Acta Cryst. C 49 , 96–97].     

Adiponitrile at 100 K

Adiponitrile, C₆H₈N₂, is a key intermediate in the synthesis of the polyamide Nylon 66 and is produced industrially on a large scale. We have determined the crystal and molecular structure of adiponitrile by single‐crystal X‐ray analysis at 100 K, a suitable crystal (m.p. 275 K) having been grown from the melt at low temperature. The compound crystallizes in the monoclinic space group P 2₁/c with Z = 2. In the crystal structure, the molecule adopts an exact C_i‐symmetric gauche –anti –gauche conformation of the C—C—C—C skeleton about an inversion centre. The molecules are densely packed, with short intermolecular contacts between the α‐H and nitrile N atoms.     

Thioacetanilide at 120 K

The title compound, C₈H₉NS, has four symmetry‐independent molecules in the asymmetric unit. These molecules link into two independent infinite N—H...S hydrogen‐bonded chains in the a‐axis direction with graph‐set notation C₂²(8). The NH—CS group adopts a trans conformation and forms a dihedral angle of about 50° with the phenyl ring. The intermolecular hydrogen‐bond energy calculated by the density functional theory (DFT) method is −14.95 kJ mol⁻¹. The correlation between the IR spectrum of this compound and the hydrogen‐bond energy is also discussed. This molecular system is of interest because of its biological function.     

Anisole at 100 K: the first crystal structure determination

The simplest alkyl aryl ether, anisole (methoxybenzene), C₇H₈O, is a feedstock chemical and is widely used in the pharmaceutical industry. The structure of anisole at 100 K, as determined by single‐crystal X‐ray analysis, is reported. A crystal (m.p. 236 K) suitable for X‐ray diffraction was obtained from the melt. The title compound crystallizes in the centrosymmetric space group P2₁/c with two molecules in the asymmetric unit (Z′ = 2). Both crystallographically distinct molecules adopt a virtually flat (C_s‐symmetric) conformation. The arrangement of the molecules in the solid state appears to be governed by close packing. No face‐to‐face π–π stacking of the molecules is observed, but rather edge‐to‐face interactions result in a herringbone packing motif.     

Meta‐barium borate,II‐BaB2O4, at 163 and 293 K

The single‐crystal X‐ray diffraction structure analysis of an excellent non‐linear optical material, viz. II‐BaB₂O₄ or Ba₃(B₃O₆)₂, has been carried out at 163 and 293 K. The two sets of structural data are compared and indicate a significant shortening of the c axial length in the unit cell at 163 K, whereas the a and b axial lengths essentially do not change.     

Acetic anhydride at 100 K: the first crystal structure determination

Acetic anhydride (ethanoic anhydride), (CH₃CO)₂O, is a widely used acetylation reagent in organic synthesis. The crystal and molecular structure, as determined by single‐crystal X‐ray analysis at 100 K, is reported for the first time. A crystal of the title compound (m.p. 200 K) suitable for X‐ray diffraction was grown from the melt at low temperature. The title compound crystallizes in the orthorhombic space group Pbcn, with Z = 4. In the crystal, the molecule adopts an exact C₂‐symmetric conformation about a crystallographic twofold axis. The molecules are densely packed. Two of the methyl H atoms form short intermolecular contacts to a neighbouring carbonyl O atom, which can be viewed as weak hydrogen bonds.