Kinetics of acyl exchange of series of N- and O-acyl salts with 4-(p-dimethylamino)styrylpyridine-N-oxide

A study has been mode of the reaction of acyl exchange between a series of N- or O-acyl salts and 4-(p-dimethylamino)styrylpyridine-N-oxide in acetonitrile solution. Values of the rate constant (k₂) and activation characteristics (E_a, G, S, and H) have been obtained for these systems.Translated from Teoreticheskaya i éksperimental'naya Khimiya, Vol. 31, No. 2, pp. 86–89, March–April, 1995.This work was performed with financial support from the State Committee of the Ukraine for Matters of Science and Technology.     

An experimental test of the double solubility rule

Vapor pressures, fusion (H_fus), and sublimation (H_s) enthalpies are reported ford, dl-2,3-dibromobutane-1,4-diol, andd,dl-dimethyl 2,3-diacetyltartrate. Values of 8.1, 7.04, 6.9, and 6.6 kcal/mol for H_fus were measured by differential scanning calorimetry and values of 28.4, 27.3, 26.2, and 25.5 kcal/mol (not corrected to 25) were calculated for H_s from the temperature dependence of vapor pressure, respectively. The vapor pressure ofdl-2,3-dibromobutane-1,4-diol, which crystallizes as a conglomerate, exceeds the vapor pressure of thed form by more than a factor of 2 over the temperature range studied. The ratio of vapor pressures ofdl- andd-dimethyl 2,3-diacetyltartrate, which crystallizes as a racemic compound, is approximately 1.5.     

What are the relative steric demands of carboxyl and methyl groups?

The relative steric demands of carboxyl and methyl groups are compared by contrasting the difference quantity H _f ^o (g, ArCOOH) — H _f ^o (g, ArCH₃) for a collection of alkylated benzoic acids and toluenes with the value for Ar=C₆H₅, the archetypical (i.e., unsubstituted) benzoic acid and toluene. We conclude that carboxyl and methyl groups are nearly the same size.     

A simplified View of δ → δ* Transition Energies in Compounds with multiple metal-metal bonds: The isolated δ — δ* manifold model

The energetics of the * transition in quadruply bonded complexes are investigated using a very simple valence-bond formalism, called the isolated * manifold (IDDM) model. In this model all electrons except for those that occupy the or * molecular orbitals are ignored, as are explicit metal-ligand interactions. The resulting equations allow the calculation of transition energies very inexpensively, albeit with poor quantitative agreement: the * transition in prototypical quadruple-bond systems is predicted to occur at energies greater than 70,000 cm¹. The model incorporates configuration interaction between the two¹ A _1g configurations (|| and |**|) to roughly the same extent as do correlated all-electron calculations. The application of the method to systems that involve relative changes in * transition energies, such as the torsional twisting of quadruple bonds, is more successful quantitatively.     

Studies on the non-isothermal kinetics of the thermal decomposition of [Cu(NBOCTB)][Cu(NO3)4]· H2O

The thermal decomposition process of the complex [Cu(NBOCTB)][Cu(NO₃)₄] H₂O has been studied by TG and DTG technique, and possible intermediates of the thermal decomposition have also been conjectured from the TG and DTG curves. The results suggest that the decomposition of the complex involves five steps: The non-isothermal kinetics of steps 1, 2 and 3 have been studied by means of the Achar and Coats-Redfern method based on TG and DTG curves. Step 1 is a Coring and Growth mechanism (n= 1), its kinetic equation may be expressed as: d/dt=Ae^–E/RT(1–). Steps 2 and 3 are both two order chemical reaction mechanisms, their kinetic equations can be expressed as: d/dt=Ae^–E/RT(1–)².This project was supported by the National Natural Science Youth Fundation of China.     

Temperature dependence of the volumetric properties of binary mixtures containing oxaalkane +n-heptane

Excess molar volumes of mixtures of n-heptane + 2,5-dioxahexane and n-heptane + 2,5,8-trioxanonane were determined from density measurentents at 5, 15, 25 and 35°C. These results allowed the following mixing quantities to be reported in all range of concentrations: , (v ^E /T) _P and (h ^E /P) _T , at 25°C. The obtained values were then compared with the calculated values by using the Flory theory and the Nitta-Chao theory of liquid mixtures. The results are discussed in terms of order or disorder creation.     

Preparation and electrochemical study of an iron(II) complex of a pentadentate planar macrocyclic ligand

The macrocycle L, prepared by template condensation of bis-6,6-(-methylhydrazino)-4-phenyl-2,2:6,2-terpyridine with glyoxal, forms a stable crystalline complex of Fe^II, [Fe(L)(H₂O)₂][PF₆]₂, which has been used as a starting material for electrochemical studies on a series of seven coordinate Fe^II complexes [Fe(L)X₂]²⁺ (X=pyridine, 4-cyanopyridine, 4-aminopyridine, 4-dimethylaminopyridine, thiophene, imidazole, 2-methylimidazole or 1,2-dimethylimidazole). Cyclic voltammetry of the aquo complex in MeCN shows three reversible one electron redox waves in the range –0.35–1.70V versus Ag/AgBF₄ reference electrode.     

Enthalpy of formation of triphenylphosphine sulfide

The first measurements of the enthalpies of combustion, sublimation, and fusion of an organo-phosphorus sulfide, triphenylphosphine sulfide, are reported: _c H _m ^o (C₁₈H₁₅PS, cr)=–(10752.58 ±2.90), _sub H _m ^o (C₁₈H₁₅PS, 403 K)=(136.80±6.09), and _fus H _m ^o (C₁₈H₁₅PS, T_m=435.92 K) =(30.53±0.21) kJ·mol^–1. Correction of the phase change enthalpies toT=298.15K and p^o =0.1 MPa results in the standard phase change enthalpy values of _sub H _m ^o (298.15 K)=(142.8 ±6.8) and _fus H _m ^o (298.15 K)=(19.28±0.21) kj·mol^–1. Accordingly, the enthalpies of formation of solid, liquid, and gaseous triphenylphosphine sulfide are derived: _f H _m ^o (C₁₈H₁₅PS, cr) =(63.20±2.56), _fH _m ^o (C₁₈H₁₅PS, l)=(82.48±2.57), and _fH _m ^o (C₁₈H₁₅PS, g)=(206.0±7.3) kJ·mol^–1. From these ancillary data, the P=S double-bond enthalpy is 394 kJ-mol^–1 and in good agreement with earlier reaction calorimetry results. These phosphorus sulfide values are compared with those for the arsenic sulfides. Plausibility arguments are given for our results.     

The use of DSC to characterize structural relaxation in thermosetting polymers

Structural relaxation in different epoxy-anhydride and epoxy-diamine resins has been investigated by differential scanning calorimetry using annealing and cooling rate experiments. The annealing experiments lead to the determination of enthalpy loss,H, at an equivalent annealing temperatureT _a=T _g-20, and for periods of annealing time, t_a, between 1 h and 4 months. The variation ofH with logt_a, defines a relaxation rate per decade,rrpd, which is very sensitive to changes of the epoxy network. The cooling rate experiments allow the determination of the apparent activation energy,h ^*. The effect of the degree of crosslinking, the addition of a reactive diluent, which acts as flexibilizer, and the length of cross-link onrrpd and h^* was studied.Financial support has been provided by DGICYT (Project no.PB93/1241). The authors are grateful to CIBA-GEIGY for supplying the epoxies and hardeners, and to HUNTSMAN CORPORATION EUROPE for supplying the JEFFAMINE*, J.M.H. wishes to acknowledge assistance for a sabbatical period from theMinisterio de Education y Ciencia.     

Effect of the organic modifier on the retention of retinoids in reversed-phase liquid chromatography

Summary The retention of retinoids in reversed-phase liquid chromatography was studied using aqueous mobile phases of different composition (methanol 94–86% and acetonityrile 92–82%) at five temperatures (40–60 °C). With both organic modifiers the effect of the molecular structure increased as the water content and the polarity of the mobile phase increased. The temperature-dependence increased in the same manner with aqueous acetonitrile mobile phases. The - interactions between the retinoids and acetonitrile diminish when the water content of the mobile phase is increased, as happens also to the hydrophobic interactions with both organic modifiers. The net effect of these changes depends on the composition of the mobile phase. There was excellent correlation of retention with all polarity parameters studied(, P, x_e, x_d, x_n, E _T ^N , _T, , _o and _d), when the calculations were made separately with methanol and acetonitrile. The volume fraction of the organic modifier, , was the only parameter describing the retention well in both organic modifiers simultaneously.     

Effects of copolymers modifying PVC and of mixing ability of components in thermal dehydrochlorination and decomposition of blends

The thermal dehydrochlorination and decomposition in air and in nitrogen of films made of PVC and blends of PVC and VC/VAC, MBS, MMA/MA or ABS were studied. Both processes take place at higher temperature in air than in nitrogen. In air, ABS and MMA/MA cause an apparent increase in the decomposition temperature of PVC, whereas in nitrogen these copolymers accelerate its decomposition.The influence of modifying copolymers on the thermal dehydrochlorination and decomposition of PVC depends not only on the type, but also on the quantity of copolymer.Small amounts of modifying copolymers in samples affect their thermal stability in the opposite way to larger contents of the copolymers. This shows that the structure of films with an incompatible mixture of PVC and copolymers plays the major role in the degradation processes.

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Zusammenfassung Die thermische Dehydrochlorierung und die Zersetzung von aus PVC und Gemischen von PVC mit VC/VAC, MBS, MMA/MA oder ABS hergestellten Filmen wurden in Luft- und StickstoffatmosphÄre untersucht. Beide Prozesse verlaufen in Luft bei höheren Temperaturen als in Stickstoff. In Luft verursachen ABS und MMA/MA eine scheinbare Erhöhung der Zersetzungstemperatur von PVC, in Stickstoff jedoch beschleunigen diese Kopolymeren die PVC-Zersetzung. Die Beeinflussung der thermischen Dehydrochlorierung und der Zersetzung von PVC durch modifizierende Kopolymere hÄngt nicht nur von der Natur, sondern auch von der Menge des Kopolymeren ab. Kleine Mengen von modifizierenden Kopolymeren beeinflussen die thermische StabilitÄt gerade in entgegengesetzter Weise wie grö\ere. Es scheint, da\ die Struktur der Filme mit inkompatiblen Mischungen von PVC und Kopolymeren in den Degradationsprozessen die Hauptrolle spielt.

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/, , / . , . / , . , . . , .

     

Thermal analysis of some cyano compounds

The thermal behaviour of the cyano compounds NaCN, K₄Fe(CN)₆ · 3H₂O, K₃Fe(CN)₆, K₃Co(CN)₆ and K₂Hg(CN)₄ has been investigated by using conventional thermal analysis techniques and infrared spectroscopy. The results indicate the absence of decomplexing reactions for all the complexes, and internal redox reactions for the compounds K₃Fe(CN)₆, K₃Co(CN)₆ and K₂Hg(CN)₄. In all the investigated cases, the formation of cyanate and carbonate is demonstrated.

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Zusammenfassung Das thermische Verhalten der Cyanoverbindungen NaCN, K₄Fe(CN)₆ · 3H₂O, K₃Fe(CN)₆, K₃Co(CN)₆ und K₂Hg(CN)₄ wurde mittels konventioneller thermischer Analysentechniken und Infrarotspektroskopie untersucht. Die Ergebnisse deuten darauf hin, daß bei allen Komplexen keine Dekomplexierungs-Reaktionen verlaufen und bei den Verbindungen K₃Fe(CN)₆, K₃Co(CN)₆ und K₂Hg(CN)₄ interne Redoxreaktionen vor sich gehen. In allen untersuchten Fällen werden Cyanat und Carbonat gebildet.

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, NaCN, K₄Fe(CN)₆ · 3H₂O, K₃Fe(CN)₆, K₃Co(CN)₆ K₂Hg(CN)₄. « » « » K₃Fe(CN)₆, K₃Co(CN)₆ K₂Hg(CN)₄. .

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Supported by the Italian MPI. Presented at Journées de Calorimetrie et Analyse Thermique, Montpellier, France, 1985.

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The authors are grateful to Mr. A. Bonetti, who ran some thermal analysis curves.     

The phenomenon of conglomerate crystallization: XXXVII: The crystallization behavior of the Cr(III) and Co(III) amine carbonates [Cr(en)2CO3]I (I) and NH4{[cis-β-Co(trien)Co3]2}(PF6)3 (II)

[Cr(en)₂CO₃]I (I), ICoO₃N₄C₅H₁₆, crystallizes from water at 21°C in space groupP2₁/c (no. 14), with lattice constantsa=7.298(4),b=8.622(8),c=17.577(6)Å,=91.29(4)°;V=1105.59 ų andd(calc; MW=359.11, Z=4)=2.157 g cm^–3. A total of 2825 data points were collected over the range of 4°250°; of these, 1855 (independent and withI3(I)) were used in the structural analysis. Data were corrected for absorption (=37.657 cm^–1) and the transmission coefficients ranged from 0.4850 to 0.9991. The finalR(F) andR _w(F) residuals were, respectively 0.134 and 0.113. The cations exist in the lattice as the enantiomeric pair () and (). NH₄{[cis--Co(trien)CO₃]₂}(PF₆)₃ (II), Co₂P₃F₁₈O₆N₉C₁₄H₄₀, crystallizes from water at 21 °C in space groupP2₁/c (no. 14), with lattice constantsa=10.397(2),b=20.292(3),c= 27.082(4) Å,=100.30(3)°;V=3545.70 ų andd(calc; MW=983.29, Z=4)=1.842 g cm^–3. A total of 3724 data were collected over the range of 4°250°; of these, 2653 (independent and withI3(I)) were used in the structural analysis. Data were corrected for absorption (=12.031 cm^–1) and the transmission coefficients ranged from 0.8326 to 0.99985. The finalR(F) andR _w (F) residuals were, respectively 0.104 and 0.124. The cations exist in the asymmetric unit as() and()[cis--Co(trien)CO₃]⁺ pairs. The three independent PF₆ ^– anions exhibit the usual high thermal motion typical of these species and the NH₄ ⁺ cation is either disordered or exhibits high thermal motion also (its H atoms could not be found in difference maps).     

Conglomerate crystallization in organic compounds II. The conformation,configuration, and spontaneous resolution of 1-phenyl-2-cyano-cyclopropane

The crystal structure of 1 -phenyi-2-cyano-cyclopropane was investigated to probe the stereochemical effects of placing different groups at the 2-position of the phenylcyclopropane moiety. The substance crystallized in space group P2₁2₁2₁ with cell constants a=16.921(3), b=7.699(2), and c=6.251(2) Å; V=814.33 ų and D (calc; z=4) =1.168 g·cm^–3. Final R(F)=0.04, using unit weights. The phenyl substituent is almost exactly in the bi-secting conformation with respect to the C-C-C angle at the point of attachment to cyclopropane. The average value of the C-C distances in the three-membered ring is 1.501 Å, which is on the low side of the ranges cited in previous studies. When we apply the additivity principle to our measured geometrical data and calculate the asymmetry parameters, the value of _cns [0.012(3)] is a little low, but within experimental error it is in accord with the value (0.017) given by Allen. However, our value of _cns (0.006(3)] is substantially lower than Allen's, which is surprising, since the bisecting phenyl ring can exert its maximum effect on the asymmetry of cyclopropane. The substance undergoes spontaneous resolution into a conglomerate of chiral crystals. Unfortunately, in the absence of anomalous scatterers, the absolute configuration could not be determined; nonetheless, the space group in which the compound crystallizes is P2₁2₁2₁, which leaves no ambiguity to the fact that the crystals are a conglomerate.     

Order and disorder in mixed metal linear chains: The homo and heterobimetallic EDTA (M(H2O)4OIOII)[M′(EDTA)] · 6H2O complexes (M = Mg,Mn, Co,Zn and Ni; M′ = Co,Ni, Cu and Zn)

Summary Polymetallic solid solutions of the ethylenediaminetetracetic acid (EDTA) and six divalent metal ions exist in the range: MgMnCoZnNiCu(EDTA) · 6H₂O where + + + + + =2, 01, 0,,2, 0, 1.This type of structure is characterized by the presence of two different octahedral carboxylate-bridged coordination sites forming infinite zig-zag chains. Visible and i.r. spectra and t.g.a. analysis show that there is occupational preference for the two coordination sites in the crystalline structure.Due to this preference, and also to the structural features, the heterobimetallic MM(EDTA) · 6H₂O compounds constitute a structurally new class of materials which can be described as ordered alternating-heterobimetallic polymeric coordination complexes.     

Kinetics of the oxidation of some polycyclic aromatic hydrocarbons by lead tetraacetate in aqueous acetic acid and perchloric acid medium

The state of metal cations in CuCr₂O₄/-Al₂O₃ catalysts under its operation in catalytic heat generators has been examined. IR spectra of adsorbed CO indicate copper ion reduction in the catalyst to Cu⁺, whose surface concentration was determined. Diffuse reflectance spectra have revealed that the initial catalyst contains Cr(VI), disappearing after reaction.

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CuCr₂O₄/-Al₂O₃ (). - CO , Cu⁺. Cu⁺. , Cr(VI), .

     

étude thermodynamique de certains médicaments

Two compounds of sulphamide type:p-amino-benzene sulphonamide (I) and 3,4-dimethylisoxazol 5-sulphanylamide (II) were studied by combustion calorimetry and by differential scanning calorimetry (DSC).The enthalpies in solid state at 298,15 K of combustion, _c H _m ^o (I)=-2788,5±1,6 kJ mol^–1, _c H _m ^o (II)=-5036±3,8 kJ mol^–1 and of formation, _f H _m ^o (I)=-458,3±1,6 kJ mol^–1, _fH _m ^o (II)=-180,1±3,8 kJ mol^–1 were determined.The thermal effects concerning the melting and phase transition of this compounds were also measured.

     

Thermodynamic study of solvent extraction of monovalent metal picrates with benzo-18-crown-6 into chloroform

Thermodynamic parameters (H _ex ⁰ and S _ex ⁰ ) for the overall extractions of monovalent metal (Na, K, Rb, and Tl) picrates with benzo-18-crown-6 (B18C6), and those (H _D,L ⁰ and S _D,L ⁰ ) for the distribution of B18C6 were determined between chloroform and water. All the extracted B18C6 complexes were l:1:1 complexes (B18C6:metal ion: picrate anion). The H _ex ⁰ and S _ex ⁰ values for all the metals are negative. Every extraction of the metal picrate with B18C6 is completely enthalpy driven. The H _D,L ⁰ and S _D,L ⁰ values of B18C6 are both positive, and the partition of B18C6 is entirely entropy driven. Enthalpy (H _ex,ip ⁰ ) and entropy changes (S _ex,ip ⁰ ) for ion-pair extractions of B18C6-metal ion complexes with picrate anions were calculated. All the H _ex,ip ⁰ and S _ex,ip ⁰ values are negative, and the ion-pair extractions are completely enthalpy driven.     

Complex polarizability as used to analyze dielectric relaxation measurements

The effect of representing dielectric properties in terms of the complex polarizability ^c = – i is examined. Loss curves ( and tan ) are shifted towards higher frequencies, revealing the existence of new relaxations and allowing the clarifications of ones already known. We have calculated the shift ratios (at maximum or tan )/ (at maximum or tan ) from the more conventional empirical equations representing the dielectric behavior. Some examples are given.     

Effect of thick fixed-charge layers on electrostatic interaction — a theoretical approach

The electrostatic interaction pressure of charged surface layers is considered qualitatively and quantitatively. In the case of mutual penetration of the surface layers in addition to Maxwell stress and osmotic resp. hydrostatic pressure an isotropic stress on the fixed charges carrying molecules of the surface layers has to be taken into account. The derivation of the pressure-distance equations is given starting from both thermodynamic/electrostatic and hydrostatic/electrostatic principles. A possible biological significance of the additional stress is discussed emphasizing its role in modifying the structure of surface layer molecules.List of symbols e ₀ elementary charge - k Boltzmann constant - n _i concentration of theith ionic species in the bulk solution - P hydrostatic pressure - P hydrostatic pressure in the bulk volume (× ) - P ^h integration constant, independent on ×:P ^h =P(h) - T absolute temperature - Z _i electrovalence of theith ionic species - thickness of the surface layer - , ₀ relative and absolute permittivities - II(×) osmotic pressure at position × - II osmotic pressure in the bulk solution (× ) - osmotic pressure in the symmetry plane of interacting identical surface layers (electric field strength equals zero) - integration constant, independent on ×: - _e ^h electrostatic component of the disjoining pressure _e ^h = _e (h) - (×) mobile charge density profile (cations and anions of the electrolyte) - (×) fixed charge density profile - ^t(x) total charge density profile ( ^t = +) - ¹(x) fixed charge density profile of one of the two surface layers ( ¹(×) 0 for 0×) - (×) electric potential profile