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AZ9RBAYCAN KIMYA JURNALI № 2 2016
51
UDC 546.815.56.86.22
NONSTOICHIOMETRY IN PbCuSbS3 COMPOUND
O.M.Aliyev, D.S.Ajdarova, S.T.Bayramova*, S.I.Aliyeva*, V.M.Ragimova
M.Nagiev Institute of Catalysis and Inorganic Chemistry, NAS of Azerbaijan
*Baku European College
zveysova@yahoo.com
Received 13.01.2016
The CuSbS2-PbS system has been studied in the interval 0-100 mol.% PbS composition and its diagram state has been ploted. The formation of the quartenary compound PbCuSbS3 congruently melting at 1125±5 K has been proved. It is established that the compound PbCuSbS3 is a phase of changing composition and its field homogeneousity is in the interval 46-52% PbS.
Keywords: nonstoichiometry, phase diagram, X-ray analysis, density.
Introduction
During the investigation of the systems CuSbS2-LnSbS3, FeSb2S4-FeLn2S4, PbS-EuBi2S4 and CuBiS2-LnBiS3 several compounds have been characterized. This work is devoted to the structural study of one of than: Cu2LnSbS7, FeLnSbS4, PbLnBi2S5 and Cu2LnBi3S7 compounds [1-5].
Experimental part
A part of the samples for measurements was synthesized by method [6], their composition was calculated from the weight change during equilibration. In addition, the samples were prepared separately by mixing the appropriate amounts of the pure elements in powder form weighed on a semi-microbalance to an accuracy of ±0.0001 mg. Starting materials were Pb (99.99%), Cu (99.999%), Sb (99.999%) and sulfur (99.99999%). The sample mass was about 1-3 g, for the density measurements, where larger samples about 3-4 g were necessary.
The mixtures were placed into quartz ampoules, which were evacuated to about 10 Pa, flushed several times which Ti guttered Ar, and finally scaled under vacuum. They were slowly (within one day) heated up to about 1220 K, kept at this temperature for one week, and cooled in the furnace. The alloys were then ground in an agate mortar, scaled again in quartz ampoules as described above, and homogenized at an appropriate. A number of samples were chemically analyzed; the deviation from the nominal composition was negligible.
DTA-measurements were performed using a thermal analyzer (NTR-70) with samples of about 1-3 g scaled under vacuum in special quartz containers. The heating rate was 5 /min, and an identical quartz crucible containing pure chromium was used as a reference. The Pt/Pt 10 at.% Rh-thermocouples were calibrated at the melting points of high purity zinc, antimony and cupper. Additionally heating curve determinations were performed on six large samples (about 5 g) with compositions in the vicinity of the melting point maximum of the 3-phase using especially designed quartz crucibles [7]. They were prepared from one master alloy whose composition was changed after the measurement several times by adding either lid, cupper or antimony. After sealing the mixture was masted to get a homogeneous alloy. The samples were heated in an electric furnace, changing the temperature by the power input, the thermo-emf signal of a Pt/Pt 10% Rh-thermocouple was simplified and recorded using the registration equipment of the DTA-apparatus described above.
X-ray measurements were made with a "Dron-3" using filtered CuXa-radiation. The lattice constants were obtained by linear regression and extrapolation to zero using the function (cos2e/sin9+cos2e/9)/2.
For the density measurements a pycno-meter with 2 ml volume was employed using water as displacement liquid. Between 3 and 4 g of the finely powdered samples were weighed into the pycnometer cell, which was then filled with water. The measurements were performed at temperature between 295 and 300 K
Results and discussions
Phase diagram.
The results of the DTA-measurements for 25 samples between 0 and 100 mol.% of PbS are collected in Table 1; all data points were evaluated from the heating curves except for a few liquidus point, where the temperatures of the effects are listed both on heating and cooling. However, because of considerable super cooling, even then the liquidus temperature cooling could only be estimated by extrapolation. Table 1 contains the solidus and liquidus temperatures for eight compositions obtained from heating curve determinations as described above.
The corresponding part of the phase diagram is shown in Figure 1.
There invariant arrests are observed in the investigated composition range, whose temperatures were fixed by additional data points outside this range.
Table 1. Results of the DTA-measurements in the CuSbS2-PbS system.
Composition, mol.% PbS Solidus, К Liquidus heating cooling, K s s a ^ 1 & p Pycnometric density, g/sm3
0.0 775 825 230 6.25
2.0 745 810 235 6.22
5.0 710 800 240 6.20
6.0 675 780 244 6.14
10 680 770 244 6.05
15 675 730 244 6.02
20 675 675 274 -
25 675 800 268 6.00
30 675 900 264 -
35 675 970 260 -
40 675 1035 256 5.98
45 - 1080 254 5.97
46 830 1090 253 5.98
48 950 1100 251 5.84
50 - 1125 250 5.75
51 - 1120 255 5.80
52 1050 1110 255 5.90
55 - 1100 255 5.91
60 955 1070 255 -
65 950 1040 75 5.92
70 950 950 72 5.94
75 960 1080 72 6.25
80 955 1190 70 6.40
85 960 1240 74 6.58
90 960 1310 72 6.60
100 - 1400 72 6.61
T, к 1400
1200
1000 800
600 h
400 CuSbS
PbS
40 60 mol. %
Fig.l. Phase diagram of the CuSbS2-PbS system (o - solidus, x - liquidus on heating or cooling resp, ▲ - one phased alloys, A - two phased alloys).
On the CuSbS2-rich side, the effect at 675 K corresponds to the eutectic between a(CuSbS2) and P(PbCuSbS3). The congruent melting point of PbCuSbS3 was found at 50 mol.% PbS and 1125± 5 K. The temperatures of the invariant arrests are in good agreement with the volume given in [8].
As far as the position of the congruent melting point is conserved, the present results agree very well with those of Bayramova et al. [8], however, their temperature maximum of 1300 K seems to be somewhat too low.
The homogeneity range of the 3-phase (PbCuSbS3) was determined [8] by based on lattice parameter measurements. As can be seen from Figure l, our PbCuSbS3-rich phase boundary is in perfect agreement with their data. Since the extension of the phase can be estimated from the first appearance of the invariant arrests at 675 K, the present results are through to be more reliable.
As possible explanation for the displacement of the melting point maximum away from the stoichiometric composition we suggest that the minimum in the integral Gibbs energy of the liquid phase is shifted considerably to the PbS-rich side.
Lattice parameters.
The lattice parameters (Table 2) were determined by X-ray measurements for two series of samples: one quenched from 675 K
O.M.ALIYEV et al.
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and one from 400 K which was also used for the density measurements.
Table 2. Lattice parameters of the phase ß(PbCuSbS3)
Composition, mol.% PbS Quenching temperature, К а, Â b, Â с, Â V, Â3
44 675 8.165 8.725 7.833 557.68
46 675 8.164 8.715 7.830 557.09
46 400 8.161 8.700 7.800 553.80
48 675 8.164 8.705 7.828 556.70
48 400 8.163 8.700 7.810 554.65
50 675 8.162 8.700 7.830 556.00
50 400 8.164 8.730 7.827 557.34
51 675 8.164 8.720 7.831 557.49
51 400 8.162 8.710 7.830 556.64
52 675 8.166 8.740 7.840 560.83
52 400 8.163 8.720 7.840 559.34
53 675 8.168 8.712 7.846 561.31
From the composition dependence shown in Figure 2 the PbS-rich phase boundary was obtained at 45 mol.% PbS (675 K) and 54 mol.% PbS (950 K). Regardless of the quenching temperature a maximum value is observed around 43.5 mol.% PbS. The values remain constant below about 43 mol.% PbS which is not quite in agreement with the results of the thermal analyses. Therefore the concentration where the slope changes should clearly indicate the beginning of the filling of the interstitial positions. Although this particular composition cannot be accurately pinpointed in Figure 2, the change of slope occurs somewhere around 52 mol.% PbS rather than exactly at the equimolecular ratio.
mol. % IliS
Fig.2. Lattice parameters of ß(solution solidus on bases PbCuSbS3) samples quenched from 675 K.
Density.
The composition dependence of the pyc-nometric density for samples quenched from 600 K is shown in Figure 3.
Fig.3. Density as a function of composition from samples quenched from 675 К (о -experimental data, x - calculated from the X-ray data).
The values are in good agreement with the results of [8-10]. It would be rather unusual if the experimentally determined densities should be higher than lattice parameters in Figure l.
Here again the curve consists of two more or less linear branches which intersect at a composition between 50.5 and 51.0 mol.% PbS rather than exactly at 50 mol.% PbS.
Also shown in Figure 3 are the theoretical densities, calculated from the lattice parameters under the assumption that above 50 mol.% PbS vacancies exist in regular cupper positions, whereas below stoichiometry interstitial positions are filled with cupper atoms. It can be clearly seen that the experimental curve is shifted to lower density values.
References
1. Алиев O.M., Агаева P.M., Гасымов В.A. Синтез и рентгенографическое исследование соединений типа Cu2LnSb3S7 (Ln=La, Nd) // Неорг. матер. 2002. T. 38. № 7. С. 784-785.
2. Алиев O.M., Агаева P.M. Фазовая диаграмма системы CuBiS2-LnBiS3 (Ln=La, Nd) // Неорг. матер. 2005. Т. 41. № 9. С. 1051-1053.
3. Гасымов В.А., Гасымова З.Н., Aliyev O.M. Синтез и рентгенографическое исследование аналогов минерала соединений типа бертъери-та FeNdSbS4 // Неорг. матер. 2004. Т. 40. № 10. С. 1247-1248.
4. Алиев O.M., Гасымов В.A., Исмаилова З.Н. Синтез и рентгенографическое исследование PbEuBi2S5 и PbYbBi2S5 - аналогов минерала ко-залита // Азерб. хим. журн. 2007. № 1. С. 116-117.
5. Smith P.P.K., Hyde B.G. The homologous series Sb2S3-wPbS structures of diantimony dilead penta-sulphide Pb2Sb2S5 and the related phase diantimony ditinpentasulphide Sn2Sb2S5 // Acta Crystallogr. Sect.B: Struct. Sci. 1983. V. 39. No 8. P. 1498-1502.
6. Weits G., Hellner E. Über komplex zusammengesetzte sulfidische. Erze VII. Zur Kristallstruktur des Cosalits, Pb2Bi2S5 // Z. Kristallogr. 1960. V. 113. P. 385-402.
7. Алиева Р.А, Байрамова С.Т., Алиев O.M. Фазовые равновесия в квазитройной системе
PbS-Cu2S-La2S3 // Хим. проблемы. 2008. № 3. С. 503-508.
8. Байрамова С.Т., Алиев O.M., Алиева Р.А, Багиева М.Р. Фазовая диаграмма системы CuSbS2-MeS (Me-Pb, Eu, Yb) //Неорг. матер. 2010. Т. 46. № 7. С. 701-707.
9. Aliyev V.O., Akhmedova N.R., Agapashayeva S. M., Aliyev O.M. Crystal growth and physicochemical properties of structural analogs of krupkaite // Inorg. Mater. 2009. V. 45. No 7. Р. 717-722.
10. Kohatsu I., Wuensch B.J. The crystal structure of aikinite, PbCuBiS3 // Acta Crystallogr., Sect. B: Structure Sci. 1971. V. 27. No. 6. P. 1245-1252.
PbCuSbS3 BIRLЭ§MЭSINDЭ QEYRI-STEXIOMETRIYA
О.М.ЭНуеу, D.S.Эjdэrova, S.T.Bayramova, S.i.Эliyeva, ^М^эЫтоуа
Си8Ь82-РЬ8 sistemi 0-100 то1.% PbS qatlhq intervalmda бyrэnilmi§ уэ опип hal diaqraml qurulmu§dur. Sistemdэ 1125±5 К^э konqruent эriyэn PbCuSbSз birlэ§mэsinin этэ1э gэldiyi subut edilmi§dir. Миэууэп ейПт^п ki, РЬСи8Ь83 birlэ§mэsi qeyri-stexiometrik оМ, dэyi§эn tэrkib1i fazadlr. Onun hэllolma sahэsi 46-52 то1.% РЬ8 ^егуаЬМа dэyi§ir.
Адаг sдzlэr: qeyri-stexiometriya, faza diarqaml, rentgenoqrafik апаШ, slxhq.
НЕСТЕХИОМЕТРИЯ В СОЕДИНЕНИИ PbCuSbS3
О.М.Алиев, Д.С.Аждарова, С.Т.Байрамова, С.И.Алиева, В.М.Рагимова
Система Си8Ь82-РЬ8 изучена в интервале концентраций 0-100 мол.% РЬ8 и построена её диаграмма состояния. Доказано образование в системе четверного соединения РЬСи8Ь83, плавящегося при 1125±5 К конгруэнтно. Установлено, что соединение РЬСи8Ь83 является фазой переменного состава, и область его гомогенности находится в интервале 46-52 мол.% РЬ8.
Ключевые слова: нестехиометрия, фазовая диаграмма, рентгенографический анализ, плотность.
