Triclinic Structure of Birefringent Crystals of K(Al0.95Cr0.05)(SO4)2⋅12H2O

The crystal structure of alum K(Al_0.95Cr_0.05)(SO₄)₂12H₂O possessing anomalous birefringence was refined in space groups Pa3 and P1 (a = b = c = 12.165(2) , R = 0.0587). The distortions of cubic symmetry are attributed to the peculiarities of the orientational disorder in the distribution of SO₄ tetrahedra and to the different degrees of distortion of the aluminum octahedra.     

Novel chromium trinuclear trifluoroacetate complexes Cr3(μ3-O)(CF3COO)6(CH3COOH)2(CF3COO) and Cr3(μ3-O)(CF3COO)6(CH3COOH)2(THF): Synthesis and crystal structure

Novel anhydrous trinuclear ₃-oxo complexes of Cr(III), Cr₃(₃-O)(CF₃COO)₆(CH₃COOH)₂(CF₃COO) (I) and of Cr(III,III,II), Cr₃(₃-O)(CF₃COO)₆(CH₃COOH)₂(THF) (II) (where THF is (CH₂)₄O) are synthesized by anodic dissolution of metallic chromium in solutions of trifluoroacetic acid in acetonitrile and in tetrahydrofuran and their structures are studied by X-ray diffraction analysis. Complex I forms orthorhombic crystals with space group Pna2₁, a = 9.778(1) , b = 16.042(2) , c = 22.851(4) , Z = 4, R ₁ = 0.0332; complex II crystallizes in monoclinic system: space group P2₁/c, a = 9.866(1) , b = 17.895(2) , c = 21.167(4) , = 100.75(2)°, Z = 4, R = 0.0422. The average Cr-(₃-O) distances in compounds I and II are almost equal (1.943(3) and 1.927(3) ). An average length of the Cr-O bond in octahedral surrounding of metal atoms is different in complexes I and II (1.985(4) and 2.003(3) , respectively), which is specified by different oxidation states of the metal atom. The CrCr distances lie in an interval of 3.366(1)–3.337(1) .__________Translated from Koordinatsionnaya Khimiya, Vol. 31, No. 4, 2005, pp. 266–272.Original Russian Text Copyright © 2005 by Glazunova, Boltalin, Troyanov.     

Entropy in dissimilarity and chirality measures

Within the prospect of quantifying the geometrical dissimilarity of molecular models on the basis of a thermodynamical formalism, the algebra of stereogenic pairing equilibria is reviewed and applied to molecular geometry: developing Rassat's proposition, an interaction energy of two figures F and F is taken as proportional tod _H ^Emphasis>/2 (F, F), whered _H denotes the Hausdorff distance. IfG is a group of rotations in E _n the geometrical version of the general equation (E) of the chemical algebra defines a distance extensionD _p(F,F) ofd _H(F,F), which is independent of the orientations of F and F, and where the coefficientp is interpreted as the reciprocal of a temperature-like parameter:p 1/T. At K (p = ), no formal entropy contributes to the definition of the uniform distanceD . At K (p = 0), the discrimination between homo- and hetero-pairing of figures by the harmonic distance Do is averaged over orientation states. Temperature-dependent chirality measuresc _p are derived fromD _p, andc is analogous to Mislow's chirality measure. If T and oT are normalized enantiomorphic triangles with coincident centroids inE ₂,c _p(T) =D _p (T, T) is calculated forp = 0 andp = , and discussed for 0 <p < . Finally, the Hausdorff interaction model is putatively related to energy profiles versus dihedral angle inmeso- anddl-molecules.     

Adsorption of Cl? ions on electrodeposited rhodium black layer (rhodized electrode) at low concentrations

The adsorption of Cl^– ions on rhodium black layer (rhodized electrodes) was studied by radiotracer technique at low Cl^– ion concentrations (c10^–5 mol dm^–3) in 1 mol dm^–3 H₂SO₄ supporting electrolyte. The specific adsorption of Cl^– ions was treated in terms of partition between solution phase and electrodeposited Rh black layer. The potential dependence of the partition coefficient is determined.     

Etude par viscosité et autodiffusion de solutions aqueuses de divers n-alkyl-benzènesulfonates

Resumé Les propriétés physico-chimiques de solutions aqueuses de différents alkyl-p-benzènesulfonates de pureté contrôlée ont été déterminées par diverses méthodes: solubilité, viscosité, autodiffusions. Les micelles formées par len-octyl-p-benzènesulfonate de sodium (C₈ SO₃ Na) et len-dodécyl-p-benzènesul-fornate de sodium (C₁₂ Na) sont globulaires dans tout le domaine de concetration exploité; les micelles (C₈ SO₃ Na + C₁₂ SO₃ Na) sont de taille proche de celles de C₈ SO₃ Na.La détermination du nombre de contre-ions liés aux micelles de C₈ SO₃ Na confirme cette structure.

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Summary Various methods, i. e. solubility, viscosity and self-diffusion have been employed to determine the physico chemical parameters of aqueous solutions of puren-alkyl-p-benzene-sulfonates. Micelles of sodiumn-octyl-p-benzene sulfonate (C₈ SO₃ Na) are of globular shape; mixed micelles formed by these compounds (C₈ SO₃ Na + C₁₂ SO₃ Na) show a very slight swelling compared with C₈ S03 Na micelles.The degree of counter-ion association of C₈ SO₃ Na micelles is in good accordance with a globular shape of the micelles.

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Zusammenfassung Löslichkeit, Viskosität und Selbst-Diffusion wurden benutzt, um physikalisch-chemische Parameter von wäßrigen Lösungen reinern-Alkyl-p-benzenesulfonate zu bestimmen. Mizellen von Natriumn-Oktylpbenzenesulfonar (C₈ SO₃ Na) haben eine globulare Form; Mischmizelle von C₈ SO₃ Na und C₁₂ SO₃ Na zeigen eine sehr geringe Quellung im Vergleich mit Mizellen von C₈ SO₃ Na.Der Grad von Gegenionenassoziation zu C₈ SO₃-Mizellen ist in guter Übereinstimmung mit einer globularen Form der Mizellen.

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Avec 6 figures et 7 tableaux

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The Lund Institute of Technology, Lund (Suède).

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Groupe de Dynamique des phases condensées, USTL.     

Über die Struktur der Bindung von Polyvinylalkohol und Borsäure

Zusammenfassung Zur Beantwortung der Frage, ob die Bindung von Polyvinylalkohol und Borsäure polyelektrolytische Eigenschaften besitzt, führte man Messungen der Funktion _sp/c=f(c) durch. Man stellte fest, daß für verschiedene Konzentrationen unter Einhaltung eines konstanten Konzentrationsverhältnisses zwischen Borsäure und Polymer die untersuchte Funktion einen für elektrolytisch nicht dissoziierende Polymeren charakteristischen Verlauf zeigt.Man arbeitete eine Verdünnungsmethode aus, die eine Spaltung der Verbindung verhütet. Mit Hilfe dieser Methode erhielt man die Kurven _sp/c vs.c, deren Maxima für Polyelektrolytlösungen charakteristisch waren.Man untersuchte die IR-Spektren von mit Wasserdampf behandelten PVAB-Filmen und stellte fest, daß die Bindung zwischen Borsäure und Polyvinylalkohol durch Wasserstoffbrücken gebildet wird.

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Summary The polyvinyl alcohol-boric acid complex was investigated in order to determine its polyelectrolytic properties. The shape of the curve _sp/c=f(c), when the mole ratio of boric acid to polyvinyl alcohol is kept constant, is characteristic for non dissociating polymers.A dilution procedure was elaborated which avoids destroying the complex in solutions, and _sp/c vs.c curves were obtained having their maxima characteristic for polyelectrolytes in solutions containing electrolytes of low molecular weight. The infrared spectra of steam treated polyvinyl alcohol-boric acid complex films were also registered and it was proved that in water solutions hydrogen bonds are responsible for the complex formation.

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Mit 7 Abbildungen     

Apparent molal volumes and heat capacities of some 1:1 electrolytes in anhydrous methanol at 25°C

A flow calorimeter and flow densimeter have been used to measure volume specific heats and densities of solutions of LiCl, LiBr, NaCl, NaBr, KF, KBr, Kl, CsF, and Bu₄NBr in anhydrous methanol at 25°C. The concentrations ranged from approximately 0.01m to close to saturation in some cases. Apparent molal heat capacities _cp and volumes _v have been evaluated and extrapolated to infinite dilution to obtain _cp ^o and _v ^o . Nearly all the heat capacities in methanol are negative. However, with the exception of the lithium halides and Bu₄NBr they are more positive than heat capacities of the corresponding salts in water. The dependence of the heat capacities on ionic radii is generally opposite in methanol solutions from that observed for aqueous solutions. In agreement with others, the _v ^o data indicate that electrostriction in methanol solutions is greater than in aqueous solutions.     

Prediction of Stability Constants for Cr(III) and Cr(II) Complexes

Regression analysis was used to derive equations for estimaing thermodynamic stability constants for complexes of Cr²⁺ (log^° ₁[Cr²⁺L] = 0.53log^° _n [H _n L]) and Cr³⁺ (log^° ₁[Cr³⁺L] = 0.88log^° _n [H _n L]) from the known protonation constants of H _n L ligands and for determining stability constants of Cr²⁺ and Cr³⁺ complexes from the available stability constants of Cu²⁺ complexes (log^° ₁[Cr²⁺L] = 0.76log^° ₁[Cu²⁺L] and log^° ₁[Cr²⁺L] = 0.60log^° ₁[Cr³⁺L], respectively). Parameters of the Panteleon–Ecka equation for calculating stability constants of Cr²⁺ complexes ( = 0.57) and Cr³⁺ complexes ( = 0.69) with two and three bidentate ligands were also determined. The ratio of logarithmic stability constants for complexes with the same metals but with different metal ionic charges was found to be approximately equal to the ratio of charges on the central ions. The stability constant of Cr(II) sulfate complex was calculated.     

Mechano-elektrochemische Effekte,VI. Einfluß der Elektrodengeometrie auf Potentialverschiebungen bei der plastischen Deformation von Kupfer und Hinweise auf die Systemorganisationen

Summary Plastic deformation of a copper electrode in an aqueous 10^–4 M Cu(ClO₄)₂ solution leads to greater potential shifts, to smaller post strain effects and to greater relaxation rates as the ratio interfacial area: volume of copper is increased. It is suggested that its system organization is improved, as the interfacial area is increased. The system organization appears also to be improved as oxidic superstructures are developing at the interface, where the highest hierarchic levels of both electrode and electrolyte are in immediate contact. Further hints as to the system organization of the whole system Cu/CuSO₄ solution are obtained from the fact that atpH=2 andc _Cu + +=10^–1 mol/l the redox potential is independent of the pretreatment of the electrode and independent of the presence of oxidic superstructures. It is underlined that the passivity due to the presence of an oxidic superstructure is maintained only atpH >2, whereas at lowerpH-values copper is more readily dissolved. It is suggested that atpH=2 the system is in an optimal state of system organization (OSO), similar to those reported in the course of phase transformations, in extremely thin metal films and in solutions at the isokinetic temperature.

     

Synthesis and X-ray structures of some mono- and binuclear ruthenium complexes with bisphosphine ligands

Summary The dinuclear complexes {RuCp*(-Cl)}₂(-dppm) (1) and {RuCp*(-Cl)}₂ (-dppe) (3) are obtained by reacting [RuCp*(³-Cl)]₄ withdppm, anddppe, respectively.1 is readily oxidized with AgCF₃SO₃, instead of chloride abstraction, to afford the dinuclear complex [{RuCp*(-Cl)}₂(-dppm)](SO₃CF₃)₂ (2) with two metal centers connected by a single Ru-Ru bond. Under the same conditions,3 decomposes to several intractable materials. Similarly to1, RuCp* (dmpe)Cl reacts with AgCF₃SO₃ to afford the Ru(III) complex [RuCp*(dmpe)Cl](SO₃CF₃) (4) without no halide abstraction. The crystal structures of2,3, and4 are presented.

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Synthese und Röntgenstrukturanalyse einiger ein- und zweikerniger Rutheniumkomplexe mit Bisphosphinliganden

Zusammenfassung Die Komplexe {RuCp*(-Cl)}₂(-dppm) (1) und {RuCp*(-Cl₂(-dppe) (3) wurden durch Umsetzung von [RuCp*(³-Cl)]₄ mitdppm bzw.dppe dargestellt.1 wird durch AgCF₃SO₃ zum zweikernigen Komplex [{RuCp*(-Cl)}₂(-dppm)](SO₃CF₃)₂ (2) oxidiert, welcher eine Ru-Ru-Metallbindung aufweist. Unter den gleiche Reaktionsbedingungen zersetzt sich3 zu undefinierten Produkten. Analog zu1 reagiert RuCp* (dmpe)Cl mit AgCF₃SO₃ zum Ru(III)-Komplex [Ru(Cp*)(dmpe)Cl](SO₃CF₃) (4) wobei es zu keiner Chloridabspaltung kommt. Von2,3, und4 wurden die Kristallstrukturen bestimmt.

     

Properties of N,N-Dimethyl-N′-(2-Hydroxybenzyl)ethylenediamine as a Ligand to Copper(II)

The acid-basic and complexing properties of N,N-dimethyl-N-(2-hydroxybenzyl)ethylenediamine (HL) in aqueous propan-2-ol were characterized by spectrophotometry, pH-metry, and mathematical simulation of equilibria in solutions (T = 25 ± 0.1°C, = 0.1 M KNO₃). Dimer H₂L₂ was found to predominate in solution at c _HL = 0.01 mol/l. Three protonated dimeric (H₃L₂ ⁺, H₄L₂ ²⁺, and H₅L₂ ³⁺), diprotonated monomeric (H₃L²⁺), and triprotonated tetrameric forms (H₇L₄ ³⁺) were detected in the system, depending on pH. At lower ligand concentrations (c _HL = 0.0015 mol/l), the solution contains both dimers and monomers of this compound. The higher dentate number of HL compared to 2-alkylaminomethylphenols allows it to form more number of both mono- and binuclear complexes ([Cu(HL)]²⁺, [Cu(HL)₂]²⁺, [CuL₂], [CuL₂OH]^–, [Cu₂(HL)₂]⁴⁺, and [Cu₂(HL)₂L₂]²⁺), making them more stable.     

Palladium(II) iminophosphine complexes

New complexes of general formula [PdCl₂(NP)] (NP = o-Ph₂PC₆H₄-CH=N-R; R = Me, ⁱ Pr, ^t Bu, NH-Me) and [Pd(NP)₂](ClO₄)₂ (NP = o-Ph₂PC₆H₄-CH=N-R; R = Me, ⁱ Pr) have been prepared by directly reacting the precursor PdCl₂(PhCN)₂ with iminophosphines (NP) in 1:1 and 1:2 molar ratios respectively. When the chloro-complex [PdCl₂(o-Ph₂PC₆H₄-CH=N ⁱ -Pr)] was treated with CF₃SO₃Ag in MeCN, the labile complex [Pd(o-Ph₂PC₆H₄-CH=N ⁱ -Pr)(MeCN)₂](CF₃SO₃)₂ was obtained in good yield. The reactivity of the new precursor towards a variety of neutral N- and P-donor ligands (py, PMe₂Ph, PMePh₂, PEt₃, bipy, dppe, 2-thpy) has been studied. The new complexes were characterized by partial elemental analyses and by spectroscopy (i.r., ¹H- and ³¹P-n.m.r.). The molecular structure of the aquo-complex [Pd(NP)(2-thpy)(H₂O)](CF₃SO₃)₂ has been determined by a single-crystal diffraction study, showing that the iminophosphine acts as a chelating ligand with coordination around the palladium atom slightly distorted from square-planar geometry.     

A solution study of complex formation between iron(III) and oxalate in dimethylsulphoxide

Summary The complex formation between iron(III) and oxalic acid (ethanedioic acid, H₂ox) has been studied by potentiometry in dimethylsulphoxide (dmso) solution. H₂ox behaves as a weak diprotic acid in such a solvent, with overall association constants: log _j1=8.551(3) and log _j2=14.242(3) at 25°C and 0.1 Mn-Bu₄NClO₄. A reliable set of overall stability constants for the iron(III)-oxalato complexes, log ₁₁=13.16(4), log ₁₂=23.66(4) and log ₁₃=30.75(4), have been obtained for the first time under identical conditions. The electrochemical behaviour of such complexes was studied in dmso at a platinum electrode. The coordination ability of oxalate towards iron(III) in dmso and water media is compared and discussed in the light of thermodynamic and structural parameters.     

Self-Consistent Calculation of Activity Coefficients and the Diffusion Layer Capacitance in Asymmetric Electrolytes

It is shown that substituting activities of individual ions for their concentrations in the equation for the ionic strength of solution substantially extends application of the first approximation of the Debye–Hückel theory for electrolytes of different valence. The obtained relationship predicts a changeover from the square root law in the charge region where the average distance between ions lis smaller than the ionic-atmosphere thickness 1/, to the cube root law, at l> 1/. The increasing deviation from experimental data upon going from LaCl₃solutions to La₂(SO₄)₃is attributed to the formation of ionic pairs LaSO₄ ⁺.     

Electroreflection Spectra of Polycrystalline Gallium in Acidic Solutions

Electroreflection spectra of solid gallium in aqueous acidic solutions have a term associated with the electromodulation of the minimum distance abetween water molecules and the ionic core of the metal, which especially heavily affects the spectra at higher frequencies f _mof modulation of potential E. The quantity da/dE –0.1 × 10^–8cm/V is determined. Spectra obtained at low f _mhave bands corresponding to charge transfer in the surface complexes formed during water chemisorption.     

Liquid-Vapor Equilibrium and Ionization of HCl in the System HCl-H2SO4-H2O at 298 K

The equilibrium pressures and compositions of the vapor over HCl-H₂SO₄-H₂O solutions with a low content of HCl and several fixed concentrations of H₂SO₄ were measured by the flow method at 298 K. The semiconcentration values of the mixed dissociation constants of HCl were calculated and extrapolated to infinite dilution.     

The effect of complexing agents on the DMF–chromium(VI) reaction. A kinetic study

The kinetics of the reduction of chromium(VI) by dimethylformamide (DMF) in the presence of ethylenediaminetetraacetic acid (EDTA) and 2,2-bipyridyl (bpy) was investigated in aqueous HClO₄ acid solutions spectrophotometrically. The experimental findings, that the reaction has an induction period followed by autoacceleration, is explained. After the reduction, chromium(III) is present as the EDTA- and bpy-complexes, although such complexes form very slowly under the same experimental conditions from chromium(III) and the EDTA and bpy, respectively. Increases in the reaction rate with increasing [EDTA] were observed, while added bpy had negligible effect on the reaction rate. The reaction is first-order each in [Cr^VI] and [H⁺]. The first-order kinetics with respect to EDTA at low concentrations shift to zero-order at higher concentrations. The reaction is considered to proceed through the formation of a very stable chromium(VI)–DMF–EDTA complex. The suggested mechanism refers only to the induction period of the reaction. The net rate of oxidation of DMF, as measured by the consumption of chromium (VI), is given by: –d[Cr^VI]/dt = kK ₁ K _b[H⁺][DMF]_T[EDTA][Cr^VI]_T/(1 + K ₁[EDTA])(1 + K _b[H⁺])     

Spin probe studies on high temperature (T >T g) microdynamics of polyamide 66 fibers

Summary Short-range segmental motions of the amorphous phase of polyamide 66 were studied by means of spin probe radicals. In a dry sample the relaxation in the temperature range 366–426 with an activation energy 27.6 kJ/mol was found. In a sample containing traces of water two processes, and relaxations, with activation energies 47.0 kJ/mol and 22.0 kJ/mol, respectively, were found. relaxation was dominant in the higher temperature range (410–460 K) while relaxation was active at lower temperatures (365–410 K).

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Zusammenfassung Die inneren, lokalen Drehbewegungen in den amorphen Bereichen des Polyamid 66 wurden mit Hilfe der Paramagnersondenmethode untersucht. Wasserfreies Polyamid 66 zeigt den-Relaxations-prozeß (die Aktivierungsenergie 27.6 kJ/Mol) im Temperaturbereich von 366 K bis 426 K, wasserhaltiges Polyamid 66 zeigt zwei Prozesse,- und-Relaxationen, deren Aktivierungsenergien 47.0 kJ/Mol und 22.0 kJ/Mol sind. Die-Relaxation dominiert in dem höheren Temperaturbereich (von 410 K bis 460 K) und die-Relaxation in dem niederen Temperaturbereich (von 365 K bis 410 K).

     

First and second thermodynamic mixing properties of ethylbenzene +n-alkanes: Experimental and theory

Isobaric expansibilities _P and isothermal compressibilities _T have been determined at 25 and 45°C for binary mixtures of ethylbenzene + n-tetradecane and + n-hexadecane and the corresponding excess functions (V ^E /T)_P and (V ^E /P)_T have also been obtained. With these data and supplementary literature values, the following second order mixing properties are also reported at 25°C: _S ^E , (V ^E /P)_T, C_V and (VT). All mixing quantities have been compared with the results obtained at 25°C by using the Prigogine-Flory-Patterson theory of liquid mixtures. The predicted values suggest that the ability of ethylbenzene as a breaker of the pure n-C_n orientations is similar to what we found for toluene and higher than for p-xylene.     

Isentropic compressibilities of univalent electrolytes in methanol at 25°C

A flow densimeter and an ultrasonic sound velocimeter have been used to measure densities and isentropic compressibilities of solutions of LiBr, NaCl, NaBr, Nal, KF, KCl, KBr, Kl, RbBr, Rbl, CsF, CsBr, Ph ₄ PBr, and NaBPh ₄ in anhydrous methanol at 25°C. the latter two electrolytes were also investigated in water at 25°C. Concentrations ranged from about 0.005 m to above 0.25m, solubility permitting. Apparent molar isentropic compressibilities, K_S,, have been calculated and extrapolated to infinite dilution to obtain K _S, ^o . The K _S, ^o values in methanol are all negative, and significantly more negative than the corresponding data in water. Additional data from the literature for acetonitrile and ethanol solutions show that K _S, ^o for the alkali metal halides become more negative in direct proportion to increasing solvent isentropic compressibility. Furthermore, the dependence of K _S, ^o in ionic size also varies in proportion to solvent isentropic compressibility. An explanation of this behavior is presented.