Beiträge zur Chemie der Oxidhalogenide von Molybdän und Wolfram,VIII. WOBr3, WOBr2-Bildungsenthalpie und thermische Zersetzung

WOBr₃ and WOBr₂ were prepared by chemical transport reactions. From the solution enthalpy of WOBr₃ in NaOH/H₂O₂ the formation enthalpy ΔH°(WOBr₃,f,298) = ?113,2(±0,9) kcal/Mol was calculated. The thermal decomposition of WOBr₃ proceeds primarly according to 2 WOBr₃ = WOBr₂ + WOBr₄. The decomposition of WOBr₂ may be described by the reaction 2 WOBr₂ = WBr₂ + WO₂Br₂. The interpretation of the decomposition equilibrium of WOBr₃ gives the values ΔH°(WOBr₂,f,298) = ?116,9(±5) kcal/Mol, and S°(WOBr₃,f,298) = 46(±5) cl.     

Beiträge zur Chemie der Oxidhalogenide von Molybdän und Wolfram. IX. Bildungsenthalpie und Sättigungsdruck des MoOBr3

From the enthalpy of solution of MoOBr₃ in NaOH/H₂O₂ the enthalpy of formation ΔH°(MoOBr₃,f,298) = ?109,5(±0,4) kcal/mol was derived. The sublimation of MoOBr₃ is connected with simultaneous decomposition (see “Inhaltsübersicht”). From the temperature function of the saturated vapor pressure the values ΔH°(subl., MoOBr₃, 298) = 36(±1,5) kcal/mol and ΔS°(subl., MoOBr₃, 298) = 56(±3) cl are calculated.     

Sättigungsdrucke,Bildungsenthalpien von WOBr4 und WO2Br2, die Reaktionsgleichgewichte 2WO2Br2 = WO3 + WOBr4 und 2WOBr4 + SiO2 = 2WO2Br2 + SiBr4

The saturation vapour pressures of WOBr₄ and WO₂Br₂ and their reaction equilibria have been determined by means of a membrane zero manometer and ampoule quenching experiments, respectively. From the pressuretemperature dependence the following sublimation data were estimated: Δ H° (subl., WOBr₄, 298) = 29.4 (± 1.0) kcal/mole; Δ H° (subl., WO₂Br₂, 298) = 36.6 (±1.5) kcal/mole; Δ S° (subl., WOBr₄, 298) = 50.1 (± 1) cl; Δ S° (subl. WO₂Br₂, 298) = 53.0 (±1.5) cl. For the decomposition reaction of solid WO₂Br₂ were obtained: Δ H° (s, 690) 37.5 (± 0.7) kcal/mole, Δ S° (s, 690) = 49.0 (± 0.5) cl; and for the decomposition of gaseous WO₂Br₂: Δ H° (g, 690) = ?29.6 (± 2.0) kcal/mole, Δ S°. (g, 690) = ?44.5 (± 1.5) cl.     

Zur thermischen Zersetzung und Sublimation des NiI2

Thermical Decomposition and Sublimation of NiI₂ In a membran manometer the thermical decomposition and the sublimation of NiI₂ was measured and in ampuls the sublimation of NiI₂ studied. From the total pressure and the sublimation pressure the enthalpy of formation ΔH°(f,NiI₂,f,298) = ?20 ± 2 kcal/mole and ΔH°(f,NiI₂,g,298) = +31.2 ± 5 kcal/mole was derived. The entropy dates are: S°(NiI₂,f,298) = 35 ± 2 cl, S°(NiI₂,g,298) = 80 ± 1 cl and S°(Ni₂I₄,g,298) = 128 ± 3 cl respectively. The Ni formed with NiI₂ an eutectical system.     

Zur Thermochemie von gasförmigem GeWO4 und GeW2O7

Thermochemistry of Gaseous GeWO₄ and GeW₂O₇ Mass spectrometric investigations with a Knudsen cell arrangement at temperatures between 1258 and 1383 K proved the existence of GeWO₄ and GeW₂O₇ as component of the vaporphase over a mechanical mixture of GeO₂ and WO₂. Using the partial pressures heats of formation (2nd law calculation) and entropies (3rd law calculation) were computed; i. e. GeWO₄: δH°₁₃₃₀ = ?149.8 kcal · mole^?1, S°₁₃₃₀ = 129.9 cal K^?1 mole^?1, GeW₂O₇: δH°_f,₁₃₃₀ = ?310.6 kcal mole^?1, S°₁₃₃₀ = 190.0 cal K^?1 mole^?1. The standard heats of formation and entropies at 298 K, calculated with estimated Cp values are: GeWO₄: δH°_f,₂₉₈ = ?181.6 kcal mole^?1, S°₂₉₈ = 85.0 cal K^?1 mole^?1; GeW₂O₇: δH°_f,₂₉₈ = ?365.8 kcal mole^?1, S°₂₉₈ = 112.1 cal K^?1 mole^?1. The thermochemical data of the GeWO₄ and GeW₂O₇ molecules which also appear at chemical transport experiments [2] with GeO₂ + WO₂, are compared with known gaseous tungstates.     

Ein Beitrag über Sr2RuO4 und Sr3Ru2O7 Zur Oktaederstreckung von M4+ in K2NiF4- und Sr3Ti2O7-Typ-Verbindungen

On the Thermal Decomposition of Hg₂I₂ and the Hg? I State Diagram Solid Hg₂I₂ decomposes congruently in Hg and HgI₂. The entropy S°(Hg₂I₂,s,298) = (55,5 ± 1) cal/K · mol and the enthalpy of formation ΔH_f°(Hg₂I₂, s, 298) = (?30,0 ± 2) kcal/mol are derived from the decomposition equilibrium. The phase diagram of the whole system Hg? I was constructed from investigations by DTA and total pressure measurements in the partial systems Hg? Hg₂I₂, Hg₂I₂? HgI₂, and HgI₂? I₂. It follows, that Hg₂I₂ melts incongruently at 297°C and decomposes in a Hg-rich and HgI₂-rich melt. The emerging miscibility gap is assumed to close at a temperature near 500°C.     

Der chemische Transport von FeP2 und FeP4 mit lod

Chemical Transport of FeP₂ and FeP₄ with Iodine Experiments on the chemical transport of FeP₂ and FeP₄ with iodine are discussed, considering the gaseous molecules I₁, I₂, FeI₂, Fe₂I₄, FeI₃, Fe₂I₆, PI₃, P₂I₄, P₄, P₂, and P. Thermodynamic calculations give δH°(298) = 56.322 kcal and ΔS°(298) = 39.5 cal/K for the reaction FeP_2,f + I₂ = FeI₂ + 0.5 P₄ and δG°(923) = 35.8 kcal for the reaction FeP_4,f + I₂ = FeI₂ + P₄.     

Equilibrium sublimation and thermodynamic properties of SnSe and SnSe2

Knudsen effusion studies of the sublimation of polycrystalline SnSe and SnSe₂, prepared by annealing and chemical vapor transport reactions, respectively, have been carried out using vacuum microbalance techniques in the temperature ranges 736–967 K and 608–760 K, respectively. From experimental mass-loss data for the sublimation reaction SnSe(s) = SnSe(g), the recommended values for the heat of formation and absolute entropy of SnSe(s) were calculated to be ΔH°_298,f = ?86.4 ± 9.9 kJ · mol^?1 and S°₂₉₈ = 89.0 ± 7.1 J · K^?1 · mol^?1. From mass-loss data for the decomposition reaction \documentclass{article}\pagestyle{empty}\begin{document}$ {\rm SnSe}_{\rm 2} ({\rm s)} = {\rm SnSe(s)} + \frac{1}{{\rm x}}{\rm Se}_{\rm x} ({\rm g) (x} = 2 - 8) $\end{document}, the recommended values for the heat of formation and absolute entropy of SnSe₂(s) were determined to be ΔH°_298,f = ?118.1 ± 15.1 kJ · mol^?1 and S°₂₉₈ = 111.8 ± 11.8 J · K^?1 mol^?1.     

Die Bildung von PPh4[WOCl4 · THF] und PPh4Cl · 4As4S3 aus W(CO)6 und PPh4[As2SCl5] sowie ihre Kristallstrukturen

Formation of PPh₄[WOCl₄ · THF] and PPh₄Cl · 4As₄S₃ from W(CO)₆ and PPh₄[As₂SCl₅] and their Crystal Structures When W(CO)₆ and PPh₄[As₂SCl₅] are irradiated with UV light in tetrahydrofurane, PPh₄[WOCl₄ · THF], PPh₄ Cl· 4As₄S₃ and PPh₄[Cl₂H] are obtained. X-ray crystal structure determinations were performed. PPh₄[WOCl₄ · THF], monoclinic, space group P2₁/c, Z = 4, a = 1207.5(2), b = 1003.7(2), c = 2642.0(5) pm, β = 114.71(1)°, R = 0.049% for 2824 reflexions; PPh₄⁺ and [WOCl₄. THF]^? ions are present, the WOCl₄ group having the shape of a tetragonal Pyramid with a short W ? O bond (169 pm) and the THF molecule being weakly associated (W? O 236 pm). PPh₄Cl · 4AsS₃, tetragonal, I4₁/a, Z = 4, a = 1742.3(3), c = 1664.5(4) pm, R = 0.066% for 1350 reflexions; it consists of separate PPh₄⁺ and Cl^? ions and As₄S₃ molecules.     

Beiträge zur Chemie der Oxidhalogenide von Molybdän und Wolfram. IV. Der Transport von MoO2 mit J2 und die Existenz von MoO2J2

The possibility to transport MoO₂ with J₂ in a temperature gradient T₂/T₁ suggests the existence of MoO₂J₂. Starting from the reaction MoO₂ + J₂ ? MoO₂J₂ in the consideration of the function of temperature for the rates of chemical transport, the values ΔH^O_R ? 28.8 (±2) kcal/mole and ΔS^O_R ? 9.0 (±2) cl are deduced. From this the values ΔH^O(MoO₂J₂, g, 298) ? ?99.5 (±3.5) kcal/mole and S^O(MoO₂J₂, g, 298) ? 86 (±3) cl are derived. The comparison of the thermodynamic data for MoO₂X₂ and WO₂X₂ (X = Cl, Br, J) leads to the conclusion, that the existence of MoO₂J₂ in the vapour phase is very probable indeed.     

Über die Reaktion von Tellur mit Wolframhalogeniden: Synthese und Struktur von Te7WOCl5, einer Verbindung mit einem polymeren Tellur-Kation

On the Reaction of Tellurium with Tungsten Halides: Synthesis and Crystal Structure of Te₇WOCl₅, a Compound with a Polymer Tellurium Cation The reaction of tellurium with WOCl₄ in the presence of a large excess of WCl₆ in a sealed evacuated glass ampoule at 150°C yields beside the main product Te₈(WCl₆)₂ a small amount of Te₇WOCl₅. The crystal structure determination (orthorhombic space group Pcca, lattice parameters at 173 K: a = 2 596.5(9) pm, b = 810.0(3) pm, c = 775.7(2) pm) shows that Te₇WOCl₅ is built of one-dimensional band shaped polymeric tellurium cations, one-dimensional associated pyramidal WOCl₄^? anions and of isolated Cl^? anions. Te₇WOCl₅ can thus be formulated as [Te₇²⁺]_n [WOCl₄^?]_n (Cl^?). The structure is closely related but not isotypic to the bromine containing analogue Te₇WOBr₅. The difference between the two structures lies in different directions of the polar [WOX₄^?]_n chains (X = Cl, Br). The strongly elongated thermal ellipsoid of one tellurium atom is shown to be caused by thermal vibration by determing the crystal structure of Te₇WOCl₅ at three different temperatures (223, 173 and 123 K). All displacement parameters of all atoms can be extrapolated to zero for 0 K.     

Zur Kristallzüchtung von Cadmiumsulfid und anderen II–VI-Verbindungen. IV. Zum Gleichgewicht zwischen Selen und Wasserstoff bei 400°C

The vapour pressure of Hg over HgSe (350–540°C) is determined by the transpiration method using N₂ and H₂ (with and without catalyst) as carrier gases. Evaluation according the equations listed in ?Inhaltsübersicht”? and regarding Se-polymerisation leads to the equilibrium function K_H2Se and to ΔH°₂₉₈ (H₂Se) = 6.4 kcal/mole. The new data are compared with literature values. The equilibrium composition of H₂Se is discussed.     

Phosphor(III)- Thiohalogenide: SP?F und SP?Br. Massenspektrometrische Untersuchungen

Phosphorus(III) Thiohalides: Sd?P? F and S?P? Br. Mass Spectrometric Investigations The compounds S?P? F and S?P? Br are formed by reaction of P(S)FBr₂ and P(S)Br₃, respectively, with silver at temperatures of about 800 K. S?P? Br is also formed by pyrolysis of P(S)Br₃ at temperatures above 298 K. Mass spectrometric equilibrium measurements lead to the heat of formation of S?P? F: ΔH°₂₉₈(SPFg) = ?260.8 kJ/mol.     

Die Gasmolekeln Pd2Al2Cl10 und PdAlCl5 als Begleiter von PdAl2Cl8

Gas Molecules Pd₂Al₂Cl₁₀ and PdAlCl₅ as Accompanists of PdAl₂Cl₈ Mass spectrometric observations using a double cell showed that the reaction of gaseous Al₂Cl₆ with solid PdCl₂ besides the known gaseous complex PdAl₂Cl₈ gives PdAlCl₅ and the unexpected complex Pd₂Al₂Cl₁₀. For the equilibrium (with ΔCp? ?1 cal/K) ΔH°(298) = 7.5 kcal/Mol and ΔS°(298) = 5.3 ± 2 cl have been obtained.     

Eine neue Methode zur Messung von temperaturabhängigen Partialdrücken in geschlossenen Systemen. Die Bestimmung der Bildungsenthalpie und -entropie von PtI2(s)

Determination of Temperature Dependent Partial Pressures in Closed Systems – a New Method. The Heat of Formation for PtI₂(s) A new method to determine temperature dependent partial pressures of gaseous species in equilibria with condensed phases in closed systems (silica ampoules) at temperatures up to 1000 °C and pressures p_i 0.01 < p_i < 10 bar is presented. It is based on the determination of the change of mass in the gasphase caused by solid-gas transition at higher temperatures of substances which are deposited at one end of the ampoule. The results of the measurements give informations about reaction mechanisms, enthalpies and entropies. The reliability of the method is demonstrated at the example of the system Pt/I₂. The heat of formation and the entropy of PtI₂(s) (δ_BH°(PtI₂(s), 298) = –51.4 kJ · mol^–1, S°(PtI₂(s), 298) = 119.3 J · K^–1 · mol^–1) are computed from experimental results. The heat of thermal decomposition of PtI₂(s) was reconsidered by Knudsen Mass Spectrometry.     

Knudsen measurements of the sublimation and the heat of formation of GeSe2 [1]

Knudsen effusion studies of the sublimation of polycrystalline GeSe₂ have been performed employing mass spectrometry in a temperature range of about 610–750 K and vacuum microbalance techniques in the temperature range 614–801 K and at pressures ranging from about 10^?7 ? 10^?4 atm. The results demonstrate that GeSe₂ vaporizes congruently under present experimental conditions according to the predominant reaction (1) GeSe₂(s) = GeSe(g) + 1/2 Se₂(g) and a minor reaction (2) GeSe₂(s) = GeSe₂(g). The mean values for the third law heat and second law entropy of reaction (1) based on direct mass-loss data are ΔH°₂₉₈ = 70.4 ± 2 kcal/mole and ΔS°₂₉₈ = 64.7 ± 2 eu. From these the standard heat of formation and absolute entropy of GeSe₂(s) were calculated to be ?21.7 ± 2 kcal/mole and 24.6 ± 2 eu, respectively.     

Fluoride und Fluorosäuren. IV. Kristallstrukturen von Bortrifluorid und seinen 1:1-Verbindungen mit Wasser und Methanol,Hydroxo- und Methoxotrifluoroborsäure

Fluorides and Fluoro Acids. IV. Crystal Structures of Boron Trifluoride and its 1:1 Compounds with Water and Methanol, Hydroxo- and Methoxotrifluoroboric Acid Solid boron trifluoride displays an enantiotropic phase transition α ? β at ?147°C. A further solid phase, γ-BF₃, is metastable or stable only just below the melting point. Its crystal structure was determined. It is monoclinic with space group P2₁/c, eight molecules in the unit cell and the lattice parameters a = 4.779, b = 14.00, c = 7.430 Å, β = 107.60° at ?131°C. Two independent trigonal planar molecules with a mean B? F bond length of 1.287 Å (1.319 Å after correction for thermal motion) form a three-dimensional packing connection with non-parallel molecular planes across intermolecular B···F contacts of in the average 2.690 Å, by which the boron atoms achieve a total coordination of five fluorine atoms with nearly trigonal bipyramidal geometry. — The crystal structures of hydroxotrifluoroboric acid (BF₃OH₂, monoclinic, P2₁/n, Z = 4, a = 7.641, b = 7.957, c = 4.864 Å, β = 94.80 at ?35°C) and methoxotrifluoroboric acid (BF₃O(CH₃)H, orthorhombic, Pbca, Z = 8, a = 7.054, b = 9.390, c = 11.547 Å at ?40°C) display unlimited three-dimensional and one-dimensional linking, respectively, of the molecules by hydrogen bonds O? H···F.     

Untersuchungen der Zersetzungsgleichgewichte und zur Phasenbreite der Molybdäntelluride

Investigation of Decomposition Equilibria and the Phase Fields of Molybdenum Tellurides The Te₂-pressure over Mo₃Te₄ and MoTe₂ as well as over equilibrium mixtures of Mo+Mo₃Te₄, Mo₃Te₄+MoTe₂, and MoTe₂+Te.l, respectively, has been measured directly between 1100 and 1373 K. No remarkable deviations from stoichiometry exist for MoTe₂ as well as for Mo₃Te₄. The coexistence pressures are for Mo/Mo₃Te₄: lg p/10⁵ Pa = 5.56—9879/T, and for Mo₃Te₄/MoTe₂: lg p/10⁵ Pa = 8.398—11790 /T. Third law enthalpies are derived: Δ_fH°(298, Mo₃Te₄) = —195.5±10 with S°(298) = 268, and Δ_fH°(298, αMoTe₂) = —89.5 ± 11 with S°(298) = 115.3 (values in kJ/mol and J mol^?1 K^?1, respectively).     

Very-low-pressure pyrolysis of N-methyl aniline and N,N-dimethyl aniline. Enthalpy of formation of the anilino and N-methyl anilino radicals

The kinetics of the thermal unimolecular decompositions of N-methyl aniline and N,N-dimethyl aniline into anilino and N-methyl anilino radicals, respectively, have been studied under very low-pressure conditions. The enthalpies of formation of both radicals, ΔH°_f,298°K(Ph?H,g) = 55.1 and ΔH°_f,298°K(Ph?Me,g) = 53.2 kcal/mol, which have been derived from the experimental data, lead to BDE(PhNH-H) = 86.4 ± 2, BDE[PhN(Me)-H] = 84.9 ± 2 kcal/mol and to a value of 16.4 kcal/mol for the stabilization energy of the PhNH radical (relative to MeNH). These results are discussed in connection with earlier work. At high temperatures, the anilino radical loses HNC and forms the very stable cyclopentadienyl radical, a decomposition comparable to that of the phenoxy radical.     

Thermische Zersetzung und Lösungskalorimetrie von Ammoniumsamariumbromiden

Thermal Decomposition and Solution Calorimetry of Ammonium Samarium Bromides The ternary pure phases on the line SmBr₃—NH₄Br in the thermodynamically equilibrium have been synthesized by solid state reactions and characterized by X‐ray powderdiffraction. The existence of a new phase (NH₄)₃SmBr₆ was demonstrated beside the known phases (NH₄)₂SmBr₅ and NH₄Sm₂Br₇. The decomposition equilibria of the ammonium samarium bromides have been investigated by total pressure measurements and the thermodynamical data of the solid phase complexes derived from the decompostion functions. The standard enthalpies of solution in 4n HBr (aq.) of the ternary phases, SmBr₃ and Sm₂O₃, were measured and on the basis of these values and known data the standard enthalpies of ammonium samarium bromides were derived. The phase diagram is constructed on the basis of DTA measurements. Data from total pressure measurements: ΔH((NH₄)₃SmBr_{6, f, 298}) = —400, 0 ± 6, 5 kcal/mol S°((NH₄)₃SmBr_{6, f, 298}) = 146, 9 ± 8 cal/K · mol ΔH((NH₄)₂SmBr_{5, f, 298}) = —340, 6 ± 5, 0 kcal/mol S°((NH₄)₂SmBr_{5, f, 298}) = 106, 0 ± 6 cal/K · mol Δ(NH₄Sm₂Br_{7, f, 298}) = —479, 4 ± 6, 0 kcal/mol S°(NH₄Sm₂Br_{7, f, 298}) = 119, 5 ± 7 cal/K · mol Data from solution calorimetry: ΔH(SmBr_{3, f, 298}) = —204, 4 ± 1, 8 kcal/mol ΔH((NH₄)₃SmBr_{6, f, 298}) = —400, 7 ± 3, 2 kcal/mol ΔH((NH₄)₂SmBr_{5, f, 298}) = —339, 6 ± 2, 6 kcal/mol ΔH(NH₄Sm₂Br_{7, f, 298}) = —475, 6 ± 4, 4 kcal/mol