J. Chem. Thermodynamics 95 (2016) 142–148 Contents lists available at ScienceDirect J. Chem. Thermodynamics journal homepage: www.elsevier.com/locate/jct Enthalpy of formation of natural hydrous copper sulfate: Chalcanthite Mira Bissengaliyeva a, Lyubov Ogorodova b,⇑, Marina Vigasina b, Lyubov Mel’chakova b, Dariya Kosova c, Igor Bryzgalov b, Dmitrii Ksenofontov b a Institute of Problems of Complex Development of Mineral Resources, Ippodromnaya Str., 5, 100019 Karaganda, Kazakhstan M.V. Lomonosov Moscow State University, Geological Faculty, MSU, Leninskie Gory, 119234 Moscow, Russia c M.V. Lomonosov Moscow State University, Chemical Faculty, MSU, Leninskie Gory, 119234 Moscow, Russia b a r t i c l e i n f o Article history: Received 3 September 2015 Received in revised form 8 December 2015 Accepted 11 December 2015 Available online 17 December 2015 Keywords: Enthalpy of formation Enthalpy of dehydration Calvet microcalorimetry Hydrous copper sulfate Chalcanthite a b s t r a c t This paper presents the results of the thermochemical study of hydrous copper sulfate CuSO45H2O performed on a high-temperature heat-flux Tian–Calvet microcalorimeter. The samples of two natural chalcanthite (Kosmurun ore deposit, Kazakhstan, and Lavrion deposit, Greece) and synthetic hydrous copper sulfate (blue vitriol) were characterized by X-ray microprobe analysis, X-ray powder diffraction, thermal analysis, FTIR and Raman spectroscopy. The enthalpy of dehydration at T = 298.15 K was measured, and the standard molar enthalpies of formation from the elements were determined by the melt solution calorimetry in accordance with Hess’s law. The values of Df H0m (T = 298.15 K) were found to be (2267.2 ± 4.1) kJmol1 for natural chalcanthite and (2272.6 ± 6.0) kJmol1 for synthetic hydrous copper sulfate (blue vitriol). Ó 2015 Published by Elsevier Ltd. 1. Introduction Natural hydrous copper sulfate CuSO45H2O, chalcanthite is a secondary mineral, which is formed in the oxidation zone of copper sulfide deposits by sedimentation from waters saturated with dissolved copper sulfate, as well as in the areas of volcanic activity. Under industrial conditions, a synthetic analog of chalcanthite (blue vitriol) is obtained by slow evaporation of an aqueous solution of copper sulfate or by dissolution of copper in sulfuric acid. The product is used in chemical and tinctorial industry, and in agriculture as a fertilizer and for pest control. For physicochemical modeling of stability of hydrous sulfates of bivalent metals and the sequence of their sedimentation in the hypergenesis zone of sulfide ores, on the evaporation barrier of water-salt basins and in hydrothermal solutions containing acidic sulfate waters near the craters of volcanoes – fumaroles, it is necessary to have reliable thermodynamic data for both hydrous and anhydrous participants of processes [1]. The data on thermodynamic properties of hydrous and anhydrous copper sulfate available in the literature are limited. In a previously reported study [2] the enthalpy of formation of anhydrous copper sulfate CuSO4 has been determined from the obtained experimental data on dissolution of copper oxide in sulfuric acid. Based on the data [3,4] on ⇑ Corresponding author. E-mail address: logor@geol.msu.ru (L. Ogorodova). http://dx.doi.org/10.1016/j.jct.2015.12.010 0021-9614/Ó 2015 Published by Elsevier Ltd. the enthalpy of dissolution of synthetic copper sulfate in water, Bergman [5] calculated the values of Df H0m (T = 298.15 K) for CuSO4. The available reference books [7–9] also used the results of the only experimental work [2]. Only one experimental value of the enthalpy of dissolution of a synthetic crystalline hydrous copper sulfate in water has been reported in the literature [4]. Based on the results of this work, the value of the enthalpy of formation of synthetic CuSO45H2O was calculated in [6], and subsequently this value was included in the reference books [7,9]. In this work, we carried out the first thermochemical study of natural chalcanthite and its synthetic analog (blue vitriol) using a Calvet microcalorimeter and obtained new data on the enthalpies of dehydration and formation of hydrous copper sulfate from its constituent elements. 2. Experimental 2.1. Materials, equipment and diagnostic methods A thermochemical study of natural chalcanthite from the oxidation zone of the Kosmurun ore deposit (the mountain ridge Genghis, Eastern Kazakhstan) (sample I) has been carried out; and for comparison we studied a sample from the Lavrion deposit (Greece) (sample II), as well as a sample of synthetic hydrous copper sulfate (blue vitriol) (sample III) (table 1). 143 M. Bissengaliyeva et al. / J. Chem. Thermodynamics 95 (2016) 142–148 TABLE 1 Provenance and mass fraction purity of substances used in this study. Substance name Chalcanthite Chalcanthite Blue vitriol Corundum Platinum Lead oxide Boric acide a b Source Natural (Kosmurun, Kazakhstan) Natural (Lavrion, Greece) Synthetic (Mosreactiv Co., Russia) Mosreactiv Co., Russia Myprom Co., Russia Mosreactiv Co., Russia Mosreactiv Co., Russia State Mass fraction purity Further treatments a Crystal Crystal Crystal Crystal Solid Powder Crystal >0.99 >0.99a >0.99b 0.999b 0.999b 0.99b 0.99b Calcination at T = 630 K Calcination at T = 630 K Calcination at T = 630 K None None Melting of the mixture of lead oxide and boric acid in a ratio 2PbO: B2O3 at T = 1073 K Purity was estimated according X-ray data. Purity grade as given by the supplier. Before study the samples of natural chalcanthite were carefully selected by hand picking under a binocular microscope. Detailed diagnostics of substances was done with use of modern physicochemical methods. Chemical analysis was carried out on a microanalyzer «CAMEBAX SX-50» (Cameca, France). To determine elemental composition, we used the analytical line Ka and the following standards: Cu – cuprite (natural); Mg – hornblende (natural); Ca – tremolite (natural); Co – CoSi (synthetic); Zn – ZnO (synthetic); Fe – spinel (natural); Pb – nodorite (natural); S – celestine (natural). All synthetic oxides were provided by company Cameca. The natural minerals were provided by A.E. Fersman Mineralogical Museum and were tested using standards provided by company Cameca using the ‘‘Camebax SX-50” and a Jeol JSM-6480LV scanning electron microscope equipped with an INCA-Wave 500 wavelength dispersive spectrometer (Jeol, Japan). The mode of operation was as follows: accelerating voltage 15 kV; probe current 30 nA. X-ray analysis was performed using a powder diffractometer «STOE-STADI MP» (Germany) equipped with a curved Ge(1 1 1) monochromator which gives strictly monochromatic CoKa1 radiation (k = 0.178897 nm). Data were collected in a regime of sequential overlapping of scanned regions using a linear position-sensitive detector with an angle of coverage of 5° at 2h with a channel width of 0.02°. IR-spectroscopic investigation was done on a Fourier spectrometer «FSM-1201» (Russia) at room temperature in the air over the range of wave numbers from (400 to 4000) cm1 with a spectral resolution of 4.0 cm1. The accuracy of the determination of the absorption bands frequencies was ±1 cm1. Specimens for the studies were prepared in the form of tablets pressed from 3 mg of mineral substance and 250 mg of KBr, as well as in the form of suspensions of mineral powder in petrolatum oil. Raman spectroscopic study was carried out on a Raman microscope «EnSpectr R532» (Russia) with a diffraction grating (1800 lines per mm) and a spectral resolution of about 6 cm1. The laser radiation wavelength was equal to 532 nm, the laser radiation power on the sample was approximately 15 mW, a single exposure time was 1 s, signal averaging was done using 50 measurements. The spectrum was obtained on a non-oriented single crystal of about 100 lm in size; a diameter of the focal laser spot was approximately 15 lm. Thermal behavior of the samples was investigated over the temperature range from room temperature to 773 K on a Derivatograph Q-1500 D (MOM, Hungary) with a heating rate of 10 Kmin1, weight of the samples was about 90 mg). 2.1.1. Chemical analysis X-ray microprobe analysis data for the composition of the samples studied are shown in table 2. The chemical formulas calculated for 2 charges coincide with the theoretical formula of CuSO45H2O. 2.1.2. X-ray diffraction The obtained X-ray diffraction patterns of natural minerals and synthetic blue vitriol are identical; in accordance with the database of the powder diffraction patterns ICDD No. 01-070-2158 [10] the studied samples are mono-mineral phases with the structure of chalcanthite (figure 1). No impurity phases were detected. 2.1.3. FTIR spectroscopy The IR-absorption spectra of all the samples studied were similar to each other, the maximum difference in the values of the wave numbers of the absorption bands did not exceed 4 cm1; the samples did not contain impurities in the noticeable amounts, and they were monomineral phases. Figure 2 shows the IR absorption spectra for the sample I (Kosmurun, Kazakhstan). The spectrum of chalcanthite prepared in a tablet with KBr (figure 2a) agrees with the spectra presented in [11,12]. It must be pointed out that this spectrum differs markedly from the spectrum of sample prepared as a suspension in petrolatum oil (figure 2b). The latter one coincides with the data [13,14] obtained by the same method. In opinion of [13], this fact may be explained by the interaction between chalcanthite and KBr, when the specimen was prepared for research. The range of wave numbers (400–4000) cm1 registered in the experiment can be divided into four non-overlapping spectral areas. The first region (3800–2600) cm1 contains a broad absorption band with a few maxima over the range of (3480–3160) cm1, corresponding to valence vibrations of water molecules present in the structure in different crystallographic positions. TABLE 2 Chemical composition of the substances studied. Oxides CuO MgO CoO ZnO FeO CaO PbO SO3 H2Ob a Sample I (Kosmurun, Kazakhstan) Sample II (Lavrion, Greece) Sample III (Synthetic) Mass fraction Ua Mass fraction Ua Mass fraction Ua 0.3207 0.0001 0.0081 0.000002 0.0074 0.00001 0.0001 0.000008 0.00001 0.0077 0.0045c 0.0076 0.000006 0.000002 0.000002 0.000002 0.3186 0.0005 0.0049 0.0004 0.0005 0.3039 0.369 0.3220 0.0003 0.0001 0.0001 0.0001 0.0002 0.0004 0.0001 0.000004 0.000008 0.000002 0.3128 0.364 0.0087 0.0045c 0.3189 0.361 0.0060 0.0045c U is the uncertainty of experimental values calculated with 0.95 level of confidence, the uncertainties are calculated on the basis of 10 determinations for each sample. b The water content was determined by the thermogravimetry method. c The uncertainty is an instrumental error (MOM recorder). 144 M. Bissengaliyeva et al. / J. Chem. Thermodynamics 95 (2016) 142–148 FIGURE 1. XRD pattern of natural chalcanthite from the Kosmurun deposit (sample I). Note that 1 angstrom = 0.1 nm. FIGURE 3. Raman spectra of natural halcanthite from the Kosmurun deposit (sample I). FIGURE 2. FTIR spectra of natural chalcanthite from the Kosmurun deposit (sample I) (obtained in transmission mode): a – in tablet of KBr; b – in petrolatum oil; c – in petrolatum oil after heating of initial mineral up to T = 630 K. The second region (1990–1500) cm1 contains the absorption band with maxima over the range of (1620–1670) cm1, which corresponds to deformation vibrations of H2O molecules and confirms the presence of water in the molecular form in the structure of the mineral. The third region (1390–760) cm1 contains absorption bands corresponding to the splitting triply degenerate valence vibration of the distorted tetrahedra [SO4]2, totally symmetric valence vibration of tetrahedra [SO4]2- and librations of H2O molecules. The fourth region (760–440) cm1 contains absorption bands corresponding to deformation vibrations of distorted tetrahedra [SO4]2. No impurity phases were detected. FIGURE 4. Thermogram of natural chalcanthite from the Kosmurun deposit (sample I). 145 1.0 0.5 6 0.5 d c b a 398.9 400.5 399.2 II III CuSO45H2O 249.67 I The accuracy of determination of the calorimetric experiment temperatures was ± 1 K. U is the uncertainty of experimental data calculated with 0.95 level of confidence. N is the number of experiments. The values of the formula weight was taken from the reference book [9]. 1.9 2.5 6 1.7 6 5 CuSO4 159.60d 40.8 40.5 40.5 Ub/kJmol1 Ub/kJmol1 d Ho(T = 630 K) Ho(T = 298.15 K) /(kJmol1) Composition of sample, formula weight/g Nc Ho(T = 630 K) Ho(T = 298.15 K) + Ddehydr.Ho(T = 630 K) /(kJmol1) 2.2.1. Tian–Calvet microcalorimetry The thermochemical study was carried out on a hightemperature heat-flux Tian–Calvet microcalorimeter «SETARAM» (France). Measurement of the enthalpy of dehydration was carried out by ‘‘the double drop” method [19]. First, a sample with a mass of (6 to 12) (±2103) mg was dropped from room temperature (298.15 K) into an empty platinum crucible in the calorimeter at the temperature 630 K, which according to the results of thermal analysis corresponds to completion of the process of total removal of water. IR absorption spectrum of the product of the heating of chalcanthite at this temperature (figure 2c) confirmed a complete dehydration of the substance and registered the change in its crystal structure. The infrared absorption spectrum of newly formed phase was obtained on suspension of a mineral powder in petrolatum oil (figure 2c) and showed signs of the onset of crystallization of chalcocyanite [10]. The thermal effect under measurement included the enthalpy increment of the sample and the enthalpy of its dehydration {Ho(T = 630 K) Ho(T = 298.15 K) + Ddehydr.Ho(T = 630 K)}. Then, the dehydrated sample was dropped again into the calorimeter at the same temperature, and we measured only the value of its enthalpy increment {Ho(T = 630 K) Ho(T = 298.15 K)}. The sample weight was controlled before and after experiments. The enthalpy of formation was determined by the melt solution calorimetry using a thermochemical cycle including the dissolution of the mineral and its constituent components [19]. We used the melt with composition 2PbO B2O3 as a solvent; the melt was prepared by melting of stoichiometric amounts of lead oxide and boric acid at T = 1073 K (weight accuracy was ±0.2 mg). On dissolution which was carried out by dropping the samples from room temperature into the melt-solvent at T = 973 K, we measured jointly the enthalpy increment of the substance and the enthalpy of its solution {Ho(T = 973 K) Ho(T = 298.15 K) + Dsol.Ho(T = 973 K)}. Masses of the samples upon dissolution were (5 to 13) Composition of sample, formula weight/g The thermochemical studies were carried out on a hightemperature heat-flux Tian–Calvet microcalorimeter ‘‘Setaram” (France) and differential scanning calorimeter «NETZSCH DSC 204 F1» (Germany) at the ambient pressure of (1004 ± 5) hPa. Number of sample 2.2. Thermochemical methods TABLE 3 Calorimetric data on dehydration of chalcanthite obtained in present work (ambient pressure P = (1004 ± 5) hPa, the uncertainty is presented as 0.95 confidence interval).a 2.1.5. Thermal analysis The thermograms obtained for the three samples of chalcanthite are identical and consistent with the literature data [18]. On the DTA curve (figure 4) we marked two endothermic effects associated with two stages of removal of water. The first of them (two-step) takes place in the temperature range (338 to 403) K and is characterized by two maxima, it corresponds to the loss of 0.27–0.30 mass fraction (about 4 molecules of water). The second stage corresponds to the lost of remaining water (0.08 mass fraction) over the range from T = (493 to 538) K. Nc 2.1.4. Raman-spectroscopy The Raman spectrum (figure 3) is similar to the Spectra shown in [14-17]. Anion [SO4]2 shows itself in the spectrum by a group of lines: a strong line 976 cm1 corresponds to the totally symmetric valence vibration of the anion; the triplet with frequencies of (1135, 1086, and 1060) cm1 corresponds to the split triply degenerate antisymmetric valence vibration; the line with a frequency of 603 cm1 belongs to the triply degenerate deformation vibration of the interior angles S–O–S; line 457 cm1 corresponds to doubly degenerate deformation vibration of the angles. The group of high-frequency lines with the frequencies of (3190, 3360, and 3472) cm1 corresponds to the valence vibrations of OH-groups (in water molecules). No impurity phases were detected. 6 4 M. Bissengaliyeva et al. / J. Chem. Thermodynamics 95 (2016) 142–148 146 M. Bissengaliyeva et al. / J. Chem. Thermodynamics 95 (2016) 142–148 TABLE 4 Results of drop solution calorimetry in the melt 2PbOB2O3 for chalcanthite obtained in the present work (ambient pressure P = (1004 ± 5) hPa, the uncertainty is presented as 0.95 confidence interval).a Number of sample Composition of sample Formula weightb/g Ho(T = 973 K) Ho(T = 298.15 K) + Dsol.Ho(T = 973 K)/(kJmol1) Nd Uc/(kJmol1) I II III a b c d CuSO4 CuSO45H2O CuSO4 CuSO4 159.60 249.67 159.60 419.7 24.1 29.5 1.0 2.9 1.3 1.9 8 7 8 6 The accuracy of determination of calorimetric experiment temperatures was ±1 K. The values of the formula weight was taken from the reference book [9]. U is the uncertainty of experimental values calculated with 0.95 level of confidence. N is the number of experiments. TABLE 5 The standard enthalpies of dehydration and of formation of pentahydrate copper sulfates. The uncertainties are calculated on the basis of the law of propagation of uncertainty. * Sample Ddehydr.Ho(T = 298.15 K)/kJmol1 Ddehydr.Ho(T = 298.15 K)/kJ(mol H2O)1 Df H0m (T = 298.15 K)/kJmol1 Sample I (Kosmurun, Kazakhstan) Sample II (Lavrion, Greece) 80.6 ± 1.8 80.0 ± 2.2 16.1 ± 0.4 16.0 ± 0.4 Sample III (Synthetic) 81.9 ± 2.5 16.4 ± 0.5 2263.3 ± 5.5 2265.4 ± 5.7 2273.0 ± 9.3* 2272.6 ± 6.0 This value was obtained using solution data for hydrous natural chalcanthite. (±2103) mg. When using (30 to 35) g of solvent during the (6–8) solution experiments the ratio of dissolved substance – melt can be attributed to an infinitely dilute solution with the enthalpy of mixing close to zero. The calibration of the instrument was carried out on each week of thermochemical studies according to the enthalpy increments when dropping the reference substances: platinum (in the experiments on dissolution at 973 K) and corundum a-Al2O3 (when studying dehydration at T = 630 K). The necessary thermochemical data for the standards were borrowed from [7]. Used in the calculations were the average values obtained for each temperature. 2.2.2. Differential scanning calorimetry Measurement of the thermal effects of the dehydration process of chalcanthite (sample I) was carried out using «NETZSCH DSC 204 F1» (Germany) in aluminum crucibles under nitrogen flow (20 mLmin1) with a heating rate of 10 Kmin1 over the temperature range from room temperature to 573 K. The instrument was calibrated according to the temperature and the enthalpy of phase transition of standard substances (C6H12, Hg, Ga, KNO3, In, Sn, Bi, 99.999% purity) [20]. Thermoanalytical system NETZSCH is located at the Chemistry Faculty of M.V. Lomonosov Moscow State University, all other equipment used is located at the Geological Faculty of M.V. Lomonosov Moscow State University. 3. Results and discussion The calorimetric results from the experiments in Tian–Calvet microcalorimeter are listed in tables 3 and 4. 3.1. The enthalpy of dehydration Using the experimental values for dehydration obtained on the Tian–Calvet microcalorimeter (table 3) and the necessary reference data for the water [21], we calculated the enthalpy of reaction (1) according to equation (2). The amount of water removed was 0.369 mass fraction (sample I), 0.364 mass fraction (sample II) and 0.361 FIGURE 5. DSC curves of natural chalcanthite from the Kosmurun deposit (sample I); thermal effects Q1 and Q2 correspond to two experimentally unseparable dehydration steps in the first stage of the water removal; thermal effect Q3 relates to the dehydration process in the second stage. mass fraction (sample III) that corresponds to a loss of about 5 water molecules in each of the samples studied. CuSO4 5H2 O ¼ CuSO4 þ 5H2 O ðlÞ; ð1Þ Ddehydr: Ho ðT ¼ 298:15 KÞ ¼ fHo ðT ¼ 630 KÞ Ho ðT ¼ 298:15 KÞ þ Ddehydr: Ho ðT ¼ 630 KÞgCuSO4 5H2 O fHo ðT ¼ 630 KÞ Ho ðT ¼ 298:15 KÞg CuSO4 5fHo ðT ¼ 630 KÞ Ho ðT ¼ 298:15 KÞg H2 O: ð2Þ The results obtained for natural samples and synthetic blue vitriol (table 5) are consistent with each other and with the value (79.45 kJmol1) calculated in [6] according to calorimetrical data on dissolving of hydrous and anhydrous copper sulfate in water [4]. The experimental results of the study of the dehydration process for natural chalcanthite (sample I) in the heating mode using differential scanning calorimetry are given in figure 5 and table 6. 147 M. Bissengaliyeva et al. / J. Chem. Thermodynamics 95 (2016) 142–148 TABLE 6 Results of DSC measurements of the dehydration thermal effect of chalcanthite (sample I). Mass of sample/mg Q1 + Q 2 Jg 2.56 3.67 2.16 TABLE 7 Thermochemical values used in the calculation of the standard enthalpies of formation of the copper sulfate pentahydrate. Q3 1 1 905.4 935.5 982.0 Component 1 kJmol Jg kJmol 225.9 233.4 245.0 297.0 306.7 319.7 74.1 76.5 79.8 Mean value: 235 ± 24* 1 Mean value: 77.0 ± 7.0* CuO(tenotite) CaO(s) CaSO4(anhydrite) Al2O3(corund) Al(OH)3(gibbsite) DHa/kJmol1 Df H0m (T = 298.15 K)b/kJmol1 c 70.10 ± 0.90 21.78 ± 0.29d 131.3 ± 1.6e 107.38 ± 0.59f 172.6 ± 1.9g 156.1 ± 2.0 635.1 ± 0.9 1434.4 ± 4.2 1675.7 ± 1.3 1293.1 ± 1.2 DH = [Ho(T = 973 K) Ho(T = 298.15 K) + Dsol.Ho(T = 973 K)]. The values of Df H0m (T = 298.15 K) are the reference values from [9]. c The values of DH were calculated using reference data on {Ho(T = 973 K) Ho(T = 298.15 K)} [9] and experimental values of Dsol.Ho(T = 973 K): c – from [19]. d The values of DH were calculated using reference data on {Ho(T = 973 K) Ho(T = 298.15 K)} [9] and experimental values of Dsol.Ho(T = 973 K): d – from [22]. e The values of DH were calculated using reference data on {Ho(T = 973 K) Ho(T = 298.15 K)} [9] and experimental values of Dsol.Ho(T = 973 K): e – from [23]. f The values of DH were calculated using reference data on {Ho(T = 973 K) Ho(T = 298.15 K)} [9] and experimental values of Dsol.Ho(T = 973 K): f – from [24]. g The value of DH is the experimental value from [25]. a b * Uncertainties are calculated with 0.95% level of confidence. The total thermal effect (Q1 + Q2) corresponds to the enthalpy of the first stage of water removal. The thermal effect Q3 corresponds to the dehydration enthalpy in the second stage. The enthalpy of complete dehydration of chalcanthite was found to be equal to (312 ± 25) kJmol1. This value relates to process of water removal in the temperature interval (330 to 530) K during heating. The value of the enthalpy of dehydration obtained by microcalorimetry method for sample I (table 5) belongs to T = 298.15 K. These data can be compared with each other after the conversion of DSC data to T = 298.15 K with considering the enthalpy of vaporization of water [21]. Estimated value of Ddehydr.Ho(T = 298.15 K) (90 kJmol1) does not contradict to the value of enthalpy obtained by means of ‘‘the double drop” method (80.6 ± 1.8 kJmol1) (table 5). 4.2. The enthalpy of formation Based on the experimental values of the dissolution of three samples of anhydrous copper sulfate (table 4) in accordance with Hess’s law, the values of their standard molar enthalpies of formation from the elements were calculated using the reaction (3) and equations (4) and (5) CuO þ CaSO4 ¼ CuSO4 þ CaO; Df H0m ðT ¼ 298:15 KÞchalcanthite ¼ Df H0m ðT ¼ 298:15 KÞdehydr:chalcanthite Drð1Þ Ho ð298:15 KÞ þ 5Df H0m ðT ¼ 298:15 KÞH2 O ðlÞ: ð6Þ The calculated values of Df H0m (T = 298.15 K) of the pentahydrates of copper sulfate studied are listed in table 5. The enthalpy of formation of chalcanthite was also determined using the data on dissolution of natural mineral (sample II) by reaction (7) and equations (8) and (9). CuO þ CaSO4 þ 3:33 AlðOHÞ3 ¼ CuSO4 5H2 O þ CaO þ 1:66 Al2 O3 ; ð7Þ Drð7Þ Ho ð298:15 KÞ ¼ DHCuO þ DHCaSO4 þ 3:33 DHAlðOHÞ3 DHchalcanthite DHCaO ð3Þ 1:66 DHAl2 O3 ; ð8Þ o Drð3Þ H ðT ¼ 298:15 KÞ ¼ DHCuO þ DHCaSO4 DHCuSO4 DHCaO; ð4Þ Df H0m ðT ¼ 298:15 KÞCuSO4 o ¼ Drð3Þ H ðT ¼ 298:15 KÞ þ þ Df H0m ðT ¼ Drð7Þ Ho ðT ¼ 298:15 KÞ þ Df H0m ðT ¼ 298:15 KÞCuO þ Df H0m ðT ¼ 298:15 KÞCaSO4 þ 3:33 Df H0m ðT ¼ 298:15 KÞAlðOHÞ3 Df H0m ðT ¼ 298:15 KÞCaSO4 ¼ 298:15 KÞCuO Df H0m ðT Df H0m ðT ¼ 298:15 KÞCaO 1:66 Df H0m ðT ¼ 298:15 KÞAl2 O3 ; ð9Þ ¼ 298:15 KÞCaO; ð5Þ where DH = {H (T = 973 K) H (T = 298.15 K) + Dsol.H (T = 973 K)} are thermochemical data for anhydrous copper sulfate (table 4) and constituent components (table 7), the values of the enthalpies of formation of the latter are shown in the same table. The enthalpy of mixing for an infinitely dilute solution is close to zero. The o Df H0m ðT ¼ 298:15 KÞchalcanthite o o derived values of Df H0m (T = 298.15 K) are equal to: (753.7 ± 5.2) (sample I), (756.4 ± 5.3) (sample II), and (761.7 ± 5.4) (sample III) kJmol1 and relate to dehydrated chalcanthite CuSO4 with signs of the onset of crystallization of chalcocyanite. These values, as might be expected, are more endothermic than the values of standard enthalpies of formation of crystalline chalcocyanite given in [7–9]: (770.9 ± 1.1), (771.4 ± 1.2) and (771.4 ± 1.3) kJmol1, respectively. The values of standard enthalpies of formation for the copper sulfate pentahydrates studied were determined using enthalpies of formation of dehydrated phases given above, and the values of enthalpies of dehydration of hydrous copper sulfates obtained in the present study (according to reaction (1)) and given at the end of the previous paragraph. The calculation was carried out based on equation (6). where DH = {Ho(T = 973 K) Ho(T = 298.15 K) + Dsol.Ho(T = 973 K)} are thermochemical data for chalcanthite (table 4) and constituent components (table 7). All the values obtained for the standard enthalpies of formation of chalcanthite (table 5) are consistent with each other within the error limits. For the synthetic sample, this value is in agreement with values for synthetic hydrous copper sulfate Df H0m (T = 298.15 K) = (2279.7 ± 3.4) kJmol1 given in the reference book [9]. The average value from three determinations for natural chalcanthite, equal (2267.2 ± 4.1) kJmol1, can be recommended as a standard value of the enthalpy of formation of natural chalcanthite. This value is different by 0.5% from that given in the reference book [9] for the synthetic analog. 4.3. Conclusions The experimental thermochemical study of chalcanthite was performed using different methods of high temperature Tian– Calvet microcalorimetry. For the first time, the value of enthalpy of dehydration was measured and the standard enthalpies of formation for natural chalcanthite and its synthetic analog (blue 148 M. Bissengaliyeva et al. / J. Chem. Thermodynamics 95 (2016) 142–148 vitriol) were obtained. The new thermodynamic values can be used for the quantitative modeling of the physicochemical conditions of weathering processes in hypergenesis zone of sulfide ores. References [1] O.L. Gas’kova, E.V. Belogub, D.V. Makarov, Geologya i Geofizika 51 (2) (2010) 222–234 (in Russian). [2] L.H. Adami, E.G. King, Heats of Formation of Anhydrous Sulfates of Cadmium, Cobalt, Copper, Nickel, and Zinc, U.S. Bur.of Mines Rept. Invest. No 6617, 1965, 10 p. [3] L.M. Gedansky, P.J. Pearce, L.G. Hepler, Can. J. Chem. 48 (1970) 1770–1773. [4] J.W. Larson, P. Cerutti, H.K. Garber, L.G. Hepler, J. Phys. Chem. 48 (11) (1968) 2902–2905. [5] G.A. Bergman, <http://www.chem.msu.su/Zn/Cu/print-CuSO4_c.html>. [6] C.W. DeKock, Thermodynamic Properties of Selected Transition Metal Sulfates and their Hydrates, U.S. Bur. Mines. Information Circular No. 8910, 1982, 45 p. [7] V.P. Glushko (Ed.), Thermal Constants of Substances, Institute of High Temperatures, Moscow, Russia, V. VI, 1972, 365 p. [8] J.D. Cox, D.D. Wagman, V.A. Medvedev, CODATA Key Values for Thermodynamics, Hemisphere Publishing Corp., New York, 1989 (www.science.uwaterloo.ca). [9] R.A. Robie, B.S. Hemingway, Thermodynamic Properties of Minerals and Related Substances at 298.15 K and 1 bar (105 Pascals) Pressure and at Higher Temperatures, U.S. Geol. Surv. Bull. No. 2131, 1995, 461 p. [10] The International Centre for Diffraction Data, PDF-2 // www.icdd.com, 2013. [11] P. Wenshi, L. Gaokui, Data Pool of the Spectra of Minerals, Publishing House of Science, Beijing, China, 1982. 129 p. [12] N.V. Chukanov, Infrared Spectra of Mineral Species: Extended Library, Springer-Verlag GmbH, Dordrecht-Heidelberg-New York-London, 2014. 1703 p. [13] A. Hezel, S.D. Ross, Spectrochim. Acta 22 (1966) 1949–1961. [14] rruff.info. [15] M. Bouchard, D.C. Smith, Spectrochim. Acta A59 (2003) 2247–2266. [16] V. Hayez, J. Guillaume, A. Hubin, H. Terryn, J. Raman Spectrosc. 35 (2004) 732– 738. [17] A. Culka, F. Košek, P. Drahota, J. Jehlička, Icarus 243 (2014) 440–453. [18] V.P. Ivanova, B.K. Kasatov, T.N. Krasavina, E.L. Rozinova, Thermal Analysis of Minerals and Rocks, Nedra, Moscow, 1974. 399 p. [19] I.A. Kiseleva, L.P. Ogorodova, L.V. Melchakova, M.R. Bisengalieva, N.S. Becturganov, Phys. Chem. Miner. 19 (1992) 322–333. [20] R.O. Grishchenko, A.L. Emelina, P.Y. Makarov, Thermochim. Acta 570 (2013) 74–79. [21] R.A. Robie, B.S. Hemingway, J.R. Fisher, Thermodynamic Properties of Minerals and Related Substances at 298.15 K and 1 bar (105 Pascals) Pressure and at Higher Temperatures, U.S. Geol. Surv. Bull. No. 1452, 1978, 456 p. [22] I.A. Kiseleva, L.P. Ogorodova, N.D. Topor, O.G. Chigareva, Geochem. Int. 16 (1979) 122–134. [23] A.R. Kotel’nikov, Yu.K. Kabalov, T.N. Zezyulya, L.V. Mel’chakova, L.P. Ogorodova, Geochem. Int. 12 (2000) 1181–1187. [24] L.P. Ogorodova, L.V. Melchakova, I.A. Kiseleva, I.A. Belitsky, Thermochim. Acta 403 (2003) 251–256. [25] L.P. Ogorodova, I.A. Kiseleva, L.V. Mel’chakova, M.F. Vigasina, E.M. Spiridinov, Russ. J. Phys. Chem. A 85 (9) (2011) 1492–1494. JCT 15-600