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1.
The important zinc borate of 2ZnO · 3B2O3 · 3H2O has been synthesized and characterized by means of chemical analysis, XRD, FT-IR, and DTA–TG techniques. The molar enthalpies of solution of H3BO3(s) in HCl · 54.561H2O, of ZnO(s) in the mixture of HCl · 54.561H2O and calculated amount of H3BO3, and of 2ZnO · 3B2O3 · 3H2O(s) in HCl · 54.604H2O were measured, respectively. With the use of the standard molar enthalpies of formation for ZnO(s), H3BO3(s), and H2O(l), the standard molar enthalpy of formation of ?(5561.7 ± 4.9) kJ · mol?1 for 2ZnO · 3B2O3 · 3H2O(s) was obtained. Thermodynamic properties of this compound were also calculated by a group contribution method.  相似文献   

2.
This paper describes a chemical model that calculates (solid + liquid) equilibria in the (m1Rb2SO4 + m2CoSO4)(aq), (m1Rb2SeO4 + m2CoSeO4)(aq), (m1Rb2SO4 + m2NiSO4)(aq), (m1Rb2SO4 + m2ZnSO4)(aq), (m1Rb2SeO4 + m2ZnSeO4)(aq), (m1Cs2SO4 + m2CoSO4)(aq), (m1Cs2SeO4 + m2CoSeO4)(aq), (m1Cs2SO4 + m2NiSO4)(aq), (m1Cs2SeO4 + m2NiSeO4)(aq), (m1Cs2SO4 + m2ZnSO4)(aq), and (m1Cs2SeO4 + m2ZnSeO4)(aq) systems, where m denotes molality at the temperature T=298.15 K. The Pitzer ion-interaction model has been used for thermodynamic analysis of the experimental osmotic and solubility data presented in the literature. The thermodynamic functions needed (binary and ternary parameters of ionic interaction, thermodynamic solubility products) have been calculated and the theoretical solubility isotherm has been plotted. The mixing parameters {θ(MN) and ψ(MNX)} have been chosen on the basis of the compositions of saturated ternary solutions and data on the binary solubility of the sulfate M2SO4. MSO4 · 6H2O double salts in water. To validate the mixing solutions model two different approaches have been used in evaluation of the ternary parameters: (I) preserving the same value of the binary mixing θ(MN) for the corresponding chloride, bromide, sulfate, and selenate systems with the same cations, and (II) with constant θ(MN) value (set equal to −0.05) for the all 11 sulfate and selenate systems. Very good agreement between experimentally determined and model predicted solubilities has been found. Important thermodynamic characteristics (thermodynamic solubility products, standard molar Gibbs free energy of formation) of the solid phases (simple salts, six sulfate – M2SO4 · MSO4 · 6H2O, and five selenate – M2SeO4 · MSeO4 · 6H2O – double salts) crystallizing in the systems under consideration are determined.  相似文献   

3.
New compounds of aspartic acid Cs(ASP) · nH2O (n = 0, 1) have been synthesized and characterized by XRD, IR and Raman spectroscopy as well as TG. The structural formula of this new compound was Cs(ASP) · nH2O (n = 0, 1). The enthalpy of solution of Cs(ASP) · nH2O (n = 0, 1) in water were determined. With the incorporation of the standard molar enthalpies of formation of CsOH(aq) and ASP(s), the standard molar enthalpy of formation of −(1202.9 ± 0.2) kJ · mol−1 of Cs(ASP) and −(1490.7 ± 0.2) kJ · mol−1 of Cs(ASP) · H2O were obtained.  相似文献   

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In this article, the experimental data of excess molar enthalpies HmE and excess molar volumes VmE are presented for a set of 20 binary mixtures comprised of the first four butyl alkanoates (methanoate to butanoate) and five α,ω-dichloroalkanes (1,2-dichloroethane to 1,6-dichlorohexane), obtained at atmospheric pressure and at a temperature of 298.15 K. The results indicate the existence of specific interactions between both kinds of compounds resulting in exothermic processes for most mixtures, except for those containing butyl methanoate which give rise to net endo/exothermic effects. The VmE are positive for mixtures of (butyl esters + 1,2-dichloroethane or 1,3-dichloropropane) and negative for the remaining ones. The change in HmE with the dichloroethane chain length for a same ester is regular although the VmE presents an irregular variation. It can, therefore, be deuced from this that the mixing process involves both effects, exothermic/endothermic and expansion/contraction, simultaneously. The behaviour of the mixtures is interpreted on the basis of the results observed and attributed to different effects taking place among the molecules studied.To improve application of the UNIFAC model using the version of Dang and Tassios, average values were recalculated again for parameters of the ester/chloride interaction, distinguishing, during its application, the functional group of the acid part of the ester. In spite of this, the model does not adequately reproduce the systems’ behaviour.  相似文献   

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The (p, ρ, T) properties and apparent molar volumes V? of ZnBr2 in ethanol at temperatures (293.15 to 393.15) K and pressures up to p = 40 MPa are reported. The measurements were made with a recently developed vibration-tube densimeter. The system was calibrated using double-distilled water, methanol, ethanol, and aqueous NaCl solutions. The experiments were carried out at molalities of m = (0.05681, 0.16958, 0.30426, 0.43835, 0.93055, 1.49016, and 1.88723) mol · kg?1 using zinc bromide. An empirical correlation for the density of (ZnBr2 + C2H5OH) with pressure, temperature, and molality has been derived. This equation of state was used to calculate other volumetric properties such as isothermal compressibility, isobaric thermal expansibility, the differences in specific heat capacities at constant pressures and volumes, apparent molar volumes of ZnBr2 in ethanol, and partial molar volumes of both components.  相似文献   

9.
Measurements of the critical parameters for {xNH3 + (1 ? x)H2O} with x = (0.9098, 0.7757, 0.6808) were carried out by using a metal-bellows variable volumometer with an optical cell. The expanded uncertainties (k = 2) in temperature, pressure, density, and composition measurements have been estimated to be less than 3.2 mK, 3.2 kPa, 0.3 kg · m?3, and 8.8 · 10?4, respectively. In each mole fraction, the critical temperature Tc was first determined on the basis of the intensity of the critical opalescence. The critical pressure pc and critical density ρc were then determined as the point at which the meniscus disappears on the isotherm at T = Tc. The expanded uncertainties (k = 2) in the present critical parameters have also been estimated. Comparisons of the present values with the literature data as well as the calculated values afforded using the equation of state are also presented.  相似文献   

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Ternary mutual diffusion coefficients (D11, D22, D12 and D21) measured by the Taylor dispersion method are reported for aqueous solutions of {levodopa (l-dopa) + β-cyclodextrin (β-CD)} solutions at T = 298.15 K and concentrations up to 0.007 mol · dm−3. Significant effects on the diffusion were observed, suggesting interactions between this carbohydrate and l-dopa. Support for this came from 1H NMR spectroscopy, which shows that these effects are due to formation of 1:1 (β-CD:l-dopa) complexes.  相似文献   

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《Solid State Sciences》2001,3(6):659-667
A new synthetic crystalline mixed alkali disilicate of composition NaKSi2O5 has been prepared by re-crystallization of a glass of corresponding composition. The compound is monoclinic, space group P21/n (a=7.3005(8) Å, b=17.389(2) Å, c=12.353(1) Å, β=91.14(1)°, V=1567.9 Å3, Z=12, Dcalc=2.52 g cm−3). The crystal used for the data collection showed twinning by pseudo-merohedry according to 2[001], a feature we took account of in the refinements. The structure was solved by direct methods and refined to a residual of R1=0.070 (170 parameters). The compound belongs to the group of tetrahedral single layer silicates. Individual sheets are parallel to (001). The stepped layers can be described as being built by the condensation of unbranched dreier double chains. The double chains in turn consist of two unbranched dreier single chains connected via common corners and exclusively containing tertiary (Q3) tetrahedra. The stacking of the layers consisting of four-, six- and eight-membered rings results in a three-dimensional structure in which the alkali cations reside in the voids between neighboring sheets. The sodium and potassium atoms show an ordered distribution among the six symmetrically independent alkali sites. The coordination numbers for Na and K vary between 4 to 5 and 6 to 7, respectively.  相似文献   

15.
Journal of Solid State Electrochemistry - Gas-tight Nd2 − xCaxZr2O7 − δ (x = 0, 0.05) pyrochlore materials have been prepared via...  相似文献   

16.
Thermodynamic properties of schapbachite (α-AgBiS2) in the phase assemblage α-AgBiS2–AgBi3S5–Bi have been studied by an EMF-technique. The EMF-measurements were made on the galvanic cell Pt(−)|Ag|AgI|AgBiS2 + AgBi3S5 + Bi|C|Pt(+), over the temperature range from (429 to 699) K. According to the EMF vs. temperature relations obtained, the enthalpy of the phase transformation from β-AgBi1+xS2 to α-AgBi1+xS2, at T = (465.55 ± 5) K, was calculated to be (7.3 ± 2.1) kJ · mol−1. New experimentally determined thermodynamic properties of the bismuth-saturated schapbachite (α-AgBi1+xS2), for each temperature region of the stable phases Bi(s) and Bi(l), were generated and analysed in detail. Based on the experimental results, Gibbs free energies of sulfidation reactions including Ag, Bi(l), S2(g), Ag2S and Bi2S3 to produce the bismuth-saturated schapbachite (α-AgBi1+xS2) have been evaluated. It has been observed that within the temperature range from (474 to 680) K, schapbachite saturated with bismuth (α-AgBi1+xS2) is thermodynamically more stable than the stoichiometric schapbachite (α-AgBiS2).  相似文献   

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A vibrating wire instrument, in which the wire was clamped at both ends, was used to measure the viscosity of {xCO2 + (1  x)CH4} with x = 0.5174 with a combined uncertainty of 0.24 μPa · s (a relative uncertainty of about 0.8 %) at temperatures T between (229 and 348) K and pressures p from (1 to 32) MPa. The corresponding mass density ρ, estimated with the GERG-2008 equation of state, varied from (20 to 600) kg · m−3. The measured viscosities were consistent within combined uncertainties with data obtained previously for this system using entirely different experimental techniques. The new data were compared with three corresponding states-type models frequently used for predicting mixture viscosities: the Extended Corresponding States (ECS) model implemented in REFPROP 9.1; the SUPERTRAPP model implemented in MultiFlash 4.4; and a corresponding states model derived from molecular dynamics simulations of Lennard Jones fluids. The measured viscosities deviated systematically from the predictions of both the ECS and SUPERTRAPP models with a maximum relative deviations of 11 % at (229 K, 600 kg · m−3) and −16 % at (258 K, 470 kg · m−3), respectively. In contrast, the molecular dynamics based corresponding states model, which is predictive for mixtures in that it does not contain any binary interaction parameters, reproduced the density and temperature dependence of the measured viscosities well, with relative deviations of less than 4.2 %.  相似文献   

19.
The acid–base properties of four aminophenol derivatives, namely m-aminophenol (L1), 4-amino-2-hydroxytoluene (L2), 2-amino-5-ethylphenol (L3) and 5-amino-4-chloro-o-cresol (L4), are studied by potentiometric and titration calorimetric measurements in NaCl(aq) (0 ? I ? 3 mol · kg?1) at T = 298.15 K. The dependence of the protonation constants on ionic strength is modelled by the Debye–Hückel, SIT (Specific ion Interaction Theory) and Pitzer equations. Therefore, the values of protonation constants at infinite dilution and the relative interaction coefficients are calculated. The dependence of protonation enthalpies on ionic strength is also determined. Distribution (2-methyl-1-propanol/aqueous solution) measurements allowed us to determine the Setschenow coefficients and the activity coefficients of neutral species. Experimental results show that these compounds behave in a very similar way, and common class parameters are reported, in particular for the dependence on ionic strength of both protonation constants and protonation enthalpies.  相似文献   

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