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1.
On the Chemical Transport of Molybdenum using HgBr2 ? Experiments and Thermochemical Calculations . Mo migrates under the influence of HgBr2 in a temperature gradient (e.g. 1 000→900°C). Besides elementary Mo we observed in some experiments the occurence of MoBr2 and MoO2 (from oxygen containing impurities) respectively. The transport behaviour (deposition sequence; deposition rates of various phases) has been enlightened by continous measurement of the mass change during the transport experiments using a special “transport balance”. Thus obtained deposition rates m(Mo) for molybdenum reached in the temperature region 800 ≤ T ≤ 1 040°C a maximum at T = 980°C independend from the starting material (Mo or Mo/MoO2 mixtures). For variable densities D of transport agent at a constant temperature (T = 950°C) increasing values for m(Mo) were observed (m(Mo) = 23 mg/h, Dmax = 8.61 mg HgBr2/cm3). Thermochemical calculation give strong evidence for the migration of Mo via the endothermal reaction . The experimental deposition rates are about half as large than the calculated values. Good agreement between calculations and experiments were obtained only assuming the presense of oxygen in the starting materials.  相似文献   

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On the Chemical Transport of Molybdenum using SbBr3 – Experiments and Thermochemical Calculations Mo migrates in a temperature gradient from the region of higher temperature to the lower temperature using SbBr3 as transport agent. For various mean transport temperatures (750 ? T ? 1000°C; T = 0,5 (T1 + T2); T2 ? T1 = 100°C) we observed small transport rates (? ? 0,6 mg/h) which rise up to 16 mg/h for higher transport agent concentrations. Small amounts of MoO2 and Sb were detected beside Mo in the sink. The observed solid phases in the sink are in agreement with thermodynamical calculations by CVTrans which also demonstrate that the formation of MoO2 and Sb as well as the transport effect of SbBr3 are caused by traces of H2O from the quartz glass wall. The sequence of deposition of Mo, MoO2 and Sb in the examined temperature range can be calculated (CVTrans) and measured with the transport balance.  相似文献   

4.
On the Chemical Transport of SiAs using Iodine — Experiments and Thermochemical Calculations Using iodine as transport agent siliconarsenide migrates in a temperature gradient. The direction of the migration depends on the chosen temperature and the concentration of the transport agent. The transport rates were measured for various transport agent concentrations (0.0002 ? C(I2) ≥ 0,02 mmol/cm3) and for various mean transport temperatures (650 ? T? ? 1 000°C). For low temperatures (e.g. T1 = 750°C→T2 = 850°C), low iodine concentrations (e.g. C(I2) = 0.001 mmol/cm3) and in the presence of H2O (from wall of silica ampoule) the following exothermic reaction is responsible for the deposition of SiAs-crystals in the sink region:
  • SiAss + 4HIg = SiI4,g + 2H2,g + 1/4As4,g
In case of higher temperatures (e.g. T2 = 1 050°C→T1 = 950°C) and higher iodine concentrations (e.g. C(I2) = 0.02 mmol/cm3) SiI4,g is the transport agent. According to model calculations the following endothermic reaction is responsible for the migration of SiAs to the region of the lower temperature:
  • SiAss + SiI4,g = 2SiI2,g + 1/4As4,g
The heterogeneous and homogenous equilibria will be discussed and an explanation of the non equilibrium transport behaviour of SiAs is given. Thermochemical data of SiAs are characterized by the quartzmembrane zero manometer technique and further verified by model calculations.  相似文献   

5.
On the Chemical Transport of CrOCl and Cr2O3 - Experiments and Model Calculations for Participation of CrOCl2,g . The migration of CrOCl in a temperature gradient (600°C→500°C) in the presence of chlorine is a result from an endothermic reaction . Above T2 = 900°C several reactions are super imposed and Cr2O3, the product of the decomposition of CrOCl, migrates following the endothermic reaction . By continously monitoring the mass changes during the complete duration of the experiment the consecutive stationary deposition reactions could be registered separately and nonstationary changes in the gasphase could be recognized. The observed decomposition of solid CrOCl into Cr2O3,s as well as CrCl3,g under equilibrium conditions is in accordance with thermochemical calculations assuming the heat of formation of CrOCl to be ΔBH = - 135.3 ± 2 [kcal/mol]. Using this value the chemical transport of CrOCl with Cl2, HCl, and HgCl2 can be described.  相似文献   

6.
Experiments and Calculations on the Chemical Transport of WO2 with HgCl2 or HgBr2 Transport experiments with WO2 or WO2 + W18O49 or W + WO2 as starting phases show that HgCl2 or HgBr2 are suitable transport agents. When using HgBr2 we observed (in customary silica ampoules) unusual high transport rates n′ > 1000 mg/h. Experimental and calculated results agree to a large extent if the presence of small amounts of H2O from the quartz glass wall and the resulting gaseous particles (for example HCl or HBr) formed under equilibrium conditions as well as an influence of convection are taken into consideration.  相似文献   

7.
On the Chemical Vapour Transport of Chromium and Manganese Monophosphide. Experimental Results and Thermochemical Calculations Using iodine as transport agent well shaped crystals of a volume up to V ≈︁ 50 mm3 (CrP) or an edgelength of approximately 1 ≈︁ 10 mm (MnP) can be grown. CrP has been deposited at the lower temperature of a temperature gradient (1050 → 950°C). At a density of the transport agent higher than D = 26 · 10−6 [mol I2/cm3] CrP and CrI2,1 coexist in the deposition region at the lower temperature. The determined composition of the condensed phases under equilibrium conditions are in accordance with thermochemical calculations assuming the heat of formation of CrP to be ΔFH= −25.5 ± 2 [kcal/mol]. Furthermore these calculations show that the solution of CrP in the gas phase leads to CrI2,g, Cr2I4,g, P2,g and P4,g, while I2,g, HIg, PI3,g and P2I4,g have to be considered as transport agents. The migration of MnP (1000 → 1100°C) results from an exothermic reaction. MnPs exists besides MnI2,1 in the source region. Thermochemical calculations are in good agreement with the experimental results and suggest the following heterogenous equilibrium to be responsible for the observed behaviour: .  相似文献   

8.
Contributions on the Thermal Behaviour of Sulphates. XVI. The Chemical Vapour Transport of Ga2(SO4)3 with Cl2 and HCl. Experimental Results and Calculations Crystals of anhydrous Ga2(SO4)3 can be grown by means of CVT (e. g. 525°C → 475°C) in the less hot region of a closed silica ampoule. We investigated the dependance of the deposition rate on the concentration of the transport agent (Cl2, HCl) and the transport temperature (475°C ≤ T ≤ 750°C; T2 > T1; ΔT = 50°C; T = 0.5(T1 + T2)). Experimental results and thermodynamic calculations on the basis of ΔFH 298 º (Ga2(SO4)3) = ?686.5 kcal/mol show a good agreement.  相似文献   

9.
Contributions on the Thermal Behaviour of Sulfates XII. The Chemical Vapour Transport of In2(SO4)3 with Cl2 and HCl. Experimental Results and Calculations By means of CVT (T1 between 500°C and 825°C; ΔT = 50°C), well shaped crystals of anhydrous In2(SO4)3 can be grown in the less hot region of a closed silica ampoule. We investigated the dependence of the deposition rate on the variation of the concentration of the transport agent (system In2(SO4)3/Cl2) and on the variation of the transport temperature (In2(SO4)3/Cl2 as well as In2(SO4)3/HCl). A comparison of the experimental results with thermodynamical calculations shows a satisfying agreement. The influence of the variation of some additional parameters (H2O from the wall of the ampoule; ΔBH(In2(SO4)3)) on the deposition rate is discussed.  相似文献   

10.
Contributions on the Thermal Behaviour of Sulfates. XIII. The Chemical Vapour Transport of Cr2(SO4)3 with Cl2 and with HCl. Experiments and Calculations Well shaped crystals (cubical or rectangular parallel-epiped respectively, edge length up to 1 mm) of rhombohedral Cr2(SO4)3 can be grown in the less hot zone of a closed silica ampoule by means of CVT using Cl2 or HCl as transport agents in endothermal transport reactions. The influence of the mean transport temperature as well as the concentration of the transport agents on the deposition rates was investigated. On the basis of thermochemical calculations an explanation of the transport mechanism is given in the present paper.  相似文献   

11.
Contributions on the Thermal Behaviour of Oxoniobates of the Transition Metals. IV The Chemical Vapour Transport of CoNb2O6 with Cl2, NH4Cl, or HgCl2. Experiments and Calculations Well shaped crystals of CoNb2O6 were obtained by CVT using Cl2 (added as PtCl2), NH4Cl or HgCl2 as transport agents (1020°C → 960°C). As a result of thermodynamic calculations the evaporation and deposition of CoNb2O6 in the presence of Cl2 can be expressed by the heterogenous endothermic equilibrium (1). The endothermic reaction (2) is responsible for the CVT of CoNb2O6 if NH4Cl is used as transport agent: The unfavourable site of the equilibrium (3) causes the small transport effect using HgCl2 as transport agent. Assuming ΔB298(CoNb2O6,s) = ?524.7 kcal/mol a satisfying agreement between thermodynamical calculation and experimental results can be reached.  相似文献   

12.
On the Migration of SiAs without using a Transport Agent – Experiments and Thermochemical Calculations SiAs migrates in a temperature gradient (T = 0.5 · (T1 + T2) = 850 to 1000°C) without adding a transport agent, into the cooler part of the silica ampoule. The migration rate depends on the temperature and the partial pressure of elemental arsenic in the silica tube. The migration rates were measured for various arsenic concentrations (0 ≤ n(As) ≤ 4 mmol/20 cm3) and for various mean transport temperatures (850 ≤ T le; 1000°C). In case of increasing the temperature the migration rate rises (e.g. T = 850°C, ?(exp.) = 0.006 mg/h; T = 1000°C, ?(exp.) = 0.044 mg/h). Adding arsenic (e.g. n(As) = 0.11 mmol, ?(exp.) = 0.067 mg/h; n(As) = 4.0 mmol, ?(exp.) = 0.82 mg/h), gives also the result of an increasing migration rate. Augmenting the pressure by adding argon as inert gas has only a small effect to the migration rate of SiAs. To explain the mechanism of the migration by using model calculations, the thermochemical data of the gaseous species SiAsg and SiAs3, g have to be estimated. According to model calculations an endothermic reaction like the following one is responsible for the migration of SiAs the region of the lower temperature: SiAss + 2 Asn, g = SiAs3, g (1 ≤ n ≥ 4).  相似文献   

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14.
On the Chemical Transport of Cr2O3 with CrI3/I2 – Experiments and Model-Calculations for Participation of CrOI2,g Gaseous chromium oxyiodides that were unknown up to now cause the migration of Cr2O3 in the temperature gradient 1 000°C→900°C when iodine (e. g. 0.1 mmol/ml) and CrI3 is added (eq. (1)). Transport agent for Cr2O3 is gaseous CrI4. With a smaller concentration of iodine (D(I2) ? 0.016 mmol/ml) and lower temperatures (e.g. T? = 850°C) the influence of H2O (from the wall of the silica ampoule) becomes more important. Under these conditions the transport of Cr2O3 is a result from the endothermic reactions (2), (3) and (4). H2,g has on the basis of the decomposition of HIg a positive difference of the solubility and H2,g should not to be considered as a transport agent. Because of the range of equilibrium-values the reaction 4 has to be taken into consideration. Estimated value of the enthalpie for CrOI2,g is fixed more precisely by thermodynamic model calculation to Δf298(CrOI2,g) = ?51.4 kcal/mol. The estimated limit of error for the enthalpie of formation is smaller than ± 5 kcal/mol. Without an addition of CrI3 is in the system Cr2O3/I2 a migration of Cr2O3 not observable.  相似文献   

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16.
On the Chemical Transport of Cr2O3 with Cl2 and with HgCl2 — Experiments and Model Calculations The migration of Cr2O3 in a temperature gradient (1 000°C → 900°C) in the presence of low concentrations of chlorine and water (from the wall of silica ampoules) is a result from the endothermic reactions (1) Cr2O3,s + H2Og + 3 Cl2,g = 2 CrO2Cl2,g + 2 HClg (2) Cr2O3,s + 1/2 O2,g + 2 Cl2,g = 2 CrO2Cl2,g With higher concentrations of chlorine, the transport reaction is (3) Cr2O3,s + 5/2 Cl2,g = 3/2 CrO2Cl2,g + 1/2 CrCl4,g The gas phase of the transport system Cr2O3/Cl2 can be reduced step by step by adding small amounts of chromium, so that CrCl3 and finally also CrCl2 become more important. Further, at a lower ratio n°(Cl)/n°(Cr) three transport reactions have to be taken into consideration; with the participation of CrOCl2,g (5). (4) Cr2O3,s + 9/2 CrCl4,g = 3/2 CrO2Cl2,g + 5 CrCl3,g (5) Cr2O3,s + 3 CrCl4,g = 3 CrOCl2,g + 2 CrCl3,g (6) Cr2O3,s + H2,g + 4 HClg = 2 CrCl2,g + 3 H2Og The reactions (1), (2) and (6) become possible through the cooperation of two transport agents at a time. The migration of Cr2O3 with HgCl2 can also be described with reactions (1) – (3). The decomposition of HgCl2 Produces the small chlorine pressure for the transport reaction. The oxidation potential of the transport agent HgCl2 is too low for the oxidation of CrIII to CrVI.  相似文献   

17.
Investigations on the Crystallization of Rhodium(III) Oxo Compounds – Chemical Vapour Transport of Rh2O3 using Chlorine Rh2O3,s migrates in chemical transport experiments with chlorine as transport agent from the higher (T2) to the lower (T1) temperature of a gradient (ΔT = 100°) due to endothermal reactions (900°C < T ≤ 1050°C; T = 0,5 · (T2 + T1)). Under the conditions of transport experiments RhCl3,s is observed in most experiments as equilibrium solid besides the sesquioxide. The transport rates for Rh2O3,s and the sublimation rates for RhCl3,s grow with increasing temperature T . The composition of the equilibrium solids, the rates of migration and the sequence of deposition (1. RhCl3,s, 2. Rh2O3,s) is well reproduced by thermodynamic model calculations. As a result of this calculations the transport behaviour of the system Rh2O3,s/Cl2 is determined by the two equilibria The influence of RhCl2,g and RhCl4,g on the transport behaviour of Rh2O3,s as well as the possible occurence of RhOCl2,g in the equilibrium gas phase will be discussed. Predictions of the transport behaviour of ternary rhodium(III) oxo compounds will be made.  相似文献   

18.
Contributions on the Thermal Behaviour of Sulfates. VIII. The Chemical Vapour Transport of FeSO4 with NH4Cl and Fe2(SO4)3 with Cl2 or NH4Cl. Experiments and Calculations Well shaped crystals of FeSO4 and Fe2(SO4)3 can be grown by CVT (T1? 650°C). We investigated the dependence of the transport rate on the concentration of the transport agent (Fe2(SO4)3/Cl2 and Fe2(SO4)3/NH4Cl) as well as on the temperature (FeSO4/NH4Cl and Fe2(SO4)3/Cl2). Using ΔfH(FeSO4) = ?220 kcal/ mol, Cp(T) = 30.1 + 9.9 · 10?3 ×T and ΔfH(Fe2(SO4)3) = ?615.4 kcal/mol a satisfying agreement between thermodynamical calculations and experimental results can be reached  相似文献   

19.
On the Chemical Transport and Sublimation of CrBr3 — Experiments and Model Calculations The migration of CrBr3 in the presence of high concentrations of bromine (for example D(Br2) = 0,05 mmol/ml; closed silica ampoules) in the investigated temperature range (T? = 625°C to 875°C; T? = 50°C) is a result from the endothermic reaction The chemical transport of CrBr3 is superimposed with the sublimation. With low concentrations of D(Br2) and high temperatures T? is the sublimation decisive participated. This is a result of the homogenous equilibrium between CrBr3,g and CrBr4,g (2a) The reaction (2a) in comparison with the chemical transport of CrCl3 with Cl2 (Gl. (2b)) is more shifted to CrBr3,g.  相似文献   

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