3D-[Pr(Im)3(ImH)]@ImH: Ein dreidimensionales Netzwerk mit vollständiger Stickstoffkoordination aus einer Imidazolschmelze / 3D-[Pr(Im)3(ImH)]@ImH: A Three-Dimensional Network with Complete Nitrogen Coordination Obtained from an Imidazole Melt

2006 ◽  
Vol 61 (7) ◽  
pp. 792-798 ◽  
Author(s):  
Klaus Müller-Buschbaum

The reaction of a melt of unsubstituted imidazole with praseodymium metal yields bright green crystals of 3D-[Pr(Im)3(ImH)]@ImH. Imidazolate ligands coordinate η1 via both N atoms their 1,3 positioning within the heterocycle being responsible for the connection of praseodymium atoms. A 3-dimensional network is formed with imidazole molecules from the melt intercalated in the crystal structure. The imidazole molecules can be released and temperature dependent reversibly be exchanged with gas molecules including argon. Thus the solvent free high temperature synthesis of rare earth elements with amine melts can also be utilized for “crystal engineering” and the synthesis of compounds with material science aspects. Furthermore 3D-[Pr(Im)3(ImH)]@ImH is the first unsubstituted imidazolate of the lanthanides.

2003 ◽  
Vol 58 (12) ◽  
pp. 722-726 ◽  
Author(s):  
A. Waśkowska ◽  
S. Dacko ◽  
Z. Czapla

Crystals of [(CH2OH)3CNH3]H2AsO4 have been grown, and X-ray diffraction analysis has shown them to be monoclinic, with space group P21. A three-dimensional network of hydrogen bonds of the type O-H. . . O and N-H. . . O forms strong cation-cation and cation-anion linkages. Stabilizing the structure, they create favourable conditions in the crystal to be polar. The temperature dependent behaviour of the dielectric permittivity, measured along three crystal axes in the range 100 - 300 K, did not show any evidence for a phase transition, while the pyroelectric properties of the crystal confirmed the lack of a centre of symmetry. These polar features locate [(CH2OH)3CNH3]H2AsO4 among the materials applicable to electrooptics and for the second harmonic generation.


1957 ◽  
Vol 30 (5) ◽  
pp. 1291-1346 ◽  
Author(s):  
David Craig

Abstract E. H. Farmer compiled a review of vulcanization which was published in 1946 as an important chapter in Volume II of “Advances in Colloid Science”. About two years later, Normann Bergem published a review under the same title. These authors dealt with the subject from rather fundamental points of view, but, because of more recent work from many laboratories and the increasing importance of elastomers, a fresh survey seems warranted. Accordingly, the present review aims to bring a part of the subject up-to-date. The viewpoint taken differs from those of Farmer and Bergem in some respects which seem rather important. For example, emphasis will be placed on the various rates of reactions including those of the scorch and reversion periods and on the importance of possible intermediates such as hydrogen sulfide and suitably terminated sulfur chains. The kinetic theory of elastomeric behavior constitutes the background against which any current treatment of vulcanization should be developed. Actually, vulcanization is a part of this background. Thus, Busse considered the following conditions necessary for the existence of rubberlike elasticity: (1) the presence of long chain molecules with freely rotating links, (2) the presence of weak secondary forces between molecules, and (3) the crosslinking of molecules into a three dimensional network. The three conditions taken together, at least in present day thinking, imply that long range elasticity results from the kinetic activity of segments which resembles yet differs from the kinetic activity of gas molecules. A segment is composed at most of only a few monomer units and is terminated at either end with another segment, a crosslink or an endgroup. When terminated with an endgroup, its kinetic activity may even detract from network behavior and then it is a defect. When terminated by a crosslink or another segment it is an integral part of the network and as such can contribute to the overall elasticity. It is more or less obvious that segments terminated by crosslinks and the crosslinks themselves should display an activity different from that of segments distant from crosslinks. Crosslinks, though relatively massive, are expected to move in a limited way (microBrownian) as a result of the kinetic activity of nearby segments. Crosslinks are necessary but are thus a sort of network defect. Those of lower functionality probably can contribute beneficially to the overall kinetic activity.


2009 ◽  
Vol 65 (3) ◽  
pp. o121-o122 ◽  
Author(s):  
Jan Janczak ◽  
Genivaldo Julio Perpétuo

The title compound, 2C6H8NO+·SeO42−·2H2O, contains 4-hydroxyanilinium cations, selenate(VI) anions and water molecules. One of the two independent cations is nearly planar (excluding the ammonium H atoms), while the other is markedly nonplanar, with the hydroxy and ammonium groups displaced from the plane of the benzene ring. This results from the antiparallel orientation of the cations, which interact through oppositely polarized ammonium and hydroxy groups. Ionic and hydrogen-bonding interactions join the oppositely charged units into a three-dimensional network. This work demonstrates the usefulness of 4-aminophenol in the crystal engineering of organic–inorganic hybrid compounds.


2013 ◽  
Vol 68 (1) ◽  
pp. 17-22 ◽  
Author(s):  
Christian Schwickert ◽  
Rainer Pöttgen

The tin-rich stannides SrCo2Sn8 and BaCo2Sn8 were synthesized from the elements in sealed tantalum tubes. They crystallize with a new structure type, space group Cccm with a=1006.0(3), b=1514.4(6), c=1385.0(6) pm for SrCo2Sn8 and a=1032.8(2), b=1516.8(3), c=1405.1(3) pm for BaCo2Sn8. The structure of the barium compound was refined on the basis of single-crystal Xray diffractometer data: wR2=0.0450, 1715 F2 values, 57 variables. The cobalt atoms have seven nearest tin neighbors with Co-Sn distances ranging from 257 to 273 pm. These CoSn7 units are condensed via common rectangular faces to [Co2Sn10] double units which build up a covalently bonded three-dimensional network through Sn-Co-Sn bridges. Larger voids left by this network are filled by the barium and the Sn2 atoms. The latter have distorted octahedral tin coordination with Sn2- Sn distances of 311 - 315 pm. The barium atoms have 13 nearest tin neighbors (352 - 399 pm Ba-Sn). Temperature-dependent magnetic susceptibility data of BaCo2Sn8 show Pauli paramagnetism.


2018 ◽  
Vol 73 (12) ◽  
pp. 979-985 ◽  
Author(s):  
Elisabeth Selb ◽  
Martina Tribus ◽  
Gunter Heymann

AbstractAt ambient conditions, PdSe2 dichalcogenides crystallize in the layered PdS2-type structure. If pressure is applied, the coordination number of palladium atoms increases and the three-dimensional pyrite-type structure with octahedral (PdSe6)4− coordination geometry is observed. For the first time, single crystals of a pyrite-type PdSe2 modification could be obtained and characterized, which were grown by multianvil high-pressure/high-temperature synthesis at 7.5 GPa and 1023 K. The crystals show the expected pyrite-type space group Pa3̅ (no. 205) and refinement results of a=613.26(3) pm, R1=0.0233, and wR2=0.0247 (all data) were received for HP-Pd0.84(1)Se2. The single-crystal data revealed significant defect formation on the palladium site with 16% vacancies, which is in line with the orthorhombic PdX2-type high-pressure polymorphs HP-Pd0.94(1)S2 and HP-Pd0.88(1)Se2. The tendency of vacancy formation on the palladium site could also be verified by EDX measurements.


2014 ◽  
Vol 70 (a1) ◽  
pp. C537-C537
Author(s):  
Sofiane Bouacida ◽  
Rafika Bouchene ◽  
Amina Khadri

Organic-inorganic hybrid compounds represent one of the most important developments in materials chemistry in recent years [1]. The role of weak intermolecular interactions in the stabilization of these hybrid systems is one of the main targets of our investigation in crystal engineering study. In continuation of our research on N-aromatic heterocyclic-metal halide salts, the X-ray crystal structures of 4-dimethylaminopyridinium (HDMAP) cation with tetrachlorocuprate (II) (1) and tetrachloroferrate (III) (2) anions is reported [2,3]. In (1), Cu(II) is situated on a twofold rotation axis (4 e). The [CuCl4]2- ions are highly distorted with a mean trans angle of 141.02(1)0as a result of hydrogen bonding interactions with two nearly planar HDMAP cations (0.0295 Å mean deviation). The crystal structure of (1) is stabilized by N–H...Cl and C–H...Cl hydrogen bonds. In the three dimensional network, cations and anions pack in the lattice so as to generate chains of [CuCl4]2- anions separated by two orientations of cation layers, which are interlocked through π–π tacking contacts between pairs of pyridine rings, with centroid–centroid distances of 3.7874 (7) Å. In (2), the protonoted 4-(dimethylamino) pyridine cation is essentially planar (the r.m.s deviation for all non-H atoms being 0.004 Å). The packing of the ionic entities is realized by alternating layers of cations and [FeCl4]- anions parallel to (010) whereby the cations are oriented in a zig-zag fashion. The crystal packing is stabilized by N–H...Cl and C–H...Cl hydrogen bonds forming a three-dimensional network.


1993 ◽  
Vol 48 (8) ◽  
pp. 1057-1064 ◽  
Author(s):  
Dieter Stäben ◽  
Dietrich Mootz

The melting diagram of the system Me4NF-H2O in the region 50-100 mol% H2O has been investigated for the first time, using DTA, DSC and temperature-dependent X-ray powder diffraction. Four crystalline hydrates Me4NF·xH2O were found, with x = 1,2.33,4 and 5, which decompose irreversibly above ca. 160°C and melt incongruently at 36°C, congruently at 46°C and again incongruently at 10°C, respectively. The crystal structure of each hydrate, except the already known one of the tetrahydrate, has been determined with MoKa diffractometer data. The monohydrate is rhombohedral with space group R3̄̄m and Z = 6 formula units per unit cell (hexagonal axes), the 2.33-hydrate monoclinic with P21/n and Z = 12, and the pentahydrate tetragonal with I4̄2 m and Z = 2. The hydrogen-bonded H2O/F- structure is an isolated centrosymmetric [F2(H2O)2]2- four-membered ring in the monohydrate, a rather open three-dimensional network in the 2.33-hydrate and a corrugated dense layer of fused fivemembered rings in the pentahydrate.


2017 ◽  
Vol 21 (02) ◽  
pp. 144-151 ◽  
Author(s):  
Rahul Soman ◽  
Subramaniam Sujatha ◽  
Chellaiah Arunkumar

Two coordination polymers, 1 and 2 were developed utilizing the favorable hexacoordinated zinc(II) center in porphyrins. Single crystal X-ray structure analysis revealed that 1 forms one dimensional array whereas 2 display three dimensional network structures. Scanning tunnelling microscopic studies have shown that compounds 1 and 2 can tunnel the electric current through the crystal lattice indicating the conducting behavior of these solid crystals. The self-assembled solid crystal 2 has shown uniform conductance whereas 1 does not. The thermal stability of these crystals were determined by TGA analysis and found to be stable up to a higher temperature of 400°C. A temperature dependent current–voltage analysis were also performed and the results indicate that the conductivity of crystals 1 and 2increases with increase in temperature. It is found that the temperature coefficient of resistance ([Formula: see text] at 100°C for 1 and 2 as -0.009 and 0.017 K[Formula: see text].


1997 ◽  
Vol 53 (3) ◽  
pp. 534-543 ◽  
Author(s):  
G. Ferguson ◽  
W. Bell ◽  
P. I. Coupar ◽  
C. Glidewell

In 1,1,1-tris(4-hydroxyphenyl)ethane, C20H18O3 (1), monoclinic la, a = 7.9781 (10), b = 18.558 (3), c = 11.1995 (13) Å, \beta–101.668 (9)°, with Z = 4, each of the hydroxyl groups acts as both a donor and an acceptor of hydrogen bonds of the type O—H...O. The molecules are thus connected into square nets, graph set R^4_4(38), pairs of which are then interwoven; the nets are themselves interconnected by further hydrogen bonds to give a continuous three-dimensional network. In 1,1,1-tris(4-hydroxyphenyl)ethane-l,4-diazabicyclo[2.2.2]octane–water (1/1/1), C20H18O3.C6H12N2.H2O (2), triclinic P\overline 1, a = 10.421 (2), b = 10.734 (2), c = 10.9756 (13) Å, \alpha = 76.645 (12), \beta 74.513 (11), \gamma = 89.305 (13)°, with Z = 2, the water molecules are linked to the trisphenol and the diamine units by O—H...O and O—H...N hydrogen bonds, respectively, to form a linear aggregate. These aggregates are linked into chains by the formation of O—H...N hydrogen bonds between the trisphenol and the neighbouring diamine; however, alongside hydrogen-bond formation between the trisphenol and the diamine, there is also partial transfer of a proton, so that the intra-chain links between trisphenol and diamine units are in fact a mixture of O—H...N and N—H...O hydrogen bonds. These chains in the [101] direction are cross-linked by further O—H...O hydrogen bonds, involving only trisphenol O atoms, which form chains in both the [010] and [001] directions, thus generating a continuous three-dimensional network. Adduct (3), 1,1,1-tris(4-hydroxyphenyl)ethane–piperazine (4/3), (C20H18O3)4.(C4H10N2)3, triclinic P\overline 1, a = 12.5049 (11), b = 12.7046 (10), c = 14.6226 (9) Å, \alpha = 113.738 (6), \beta = 100.839 (6), \gamma = 102.438 (7)°, with Z = 1, has two independent trisphenol molecules in general positions and three independent piperazine molecules lying about centres of inversion. The five independent components of the asymmetric unit are linked together by means of three O—H...N and one O—H...O hydrogen bonds to form an open aggregate containing no hydrogen-bonded rings. These aggregates are connected into three sets of interlinked chains in the [010], [001] and [\overline 110] directions: the [010] and [\overline 110] chains employ only O—H...O hydrogen bonds, while the [001] chains employ both O—H...N and N—H...O hydrogen bonds. Additionally, the inversion symmetry at each piperazine unit gives rise to further interlinks.


2019 ◽  
Vol 799 ◽  
pp. 165-170
Author(s):  
Le Liu ◽  
Tatevik Minasyan ◽  
Sofiya Aydinyan ◽  
Irina Hussainova

The concept of manufacturing of near-net-shaped three-dimensional ceramic-based parts with the required geometry is motivated by design and development of advanced ceramics for high-performance applications. It is an incontestable fact, that additive manufacturing (AM), as an intensively developing smart technology, owns a unique position in modern-day product development, proposing new waste-less, cost effective and environmentally friendly pathways for manufacturing of arbitrary geometries. This work takes a new step for the synthesis of TiC/TiN lattice with geometrically defined porosity by three stage strategy (i) preparation of a TiC/Ti composite by energy saving self-propagating high-temperature synthesis (SHS) technique. (ii) preparation of designed 3D TiC/Ti shape by selective laser melting (SLM); (iii) nitridation of the consolidated samples in nitrogen environment. The influence of synthesis and nitridation conditions on the characteristics of both the powder and produced parts was investigated; set of parameters has been adjusted and optimized. Phase composition and microstructure features were examined after each procedure to reveal the physicochemical transformations and morphology evolution of the composites.


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