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1.
Chemical Vapor Transport of Intermetallic Systems. 8. Chemical Transport of Titaniumgermanides By means of chemical vapor transport using iodine as transport agent in the System Ti/Ge the compounds TiGe2 and Ti5Ge3 have been prepared in form of single crystals. Unexpectedly the phase Ti6Ge5 could not be deposited from the vapor phase. The experiments show in contrast to the literature that Ti6Ge5 is at 700 °C thermodynamic unstable. Chemical vapor transport is a suitable method to determine coexistence conditions of intermetallic compounds.  相似文献   

2.
The chemical transport of LaPO4 (1400 → 1200°K) is discussed on a thermodynamical basis and experimentally checked. Br2 + PBr3 used as transport agents give good transportrates. Br2 + CO and Br2 + C are also suitable transportsystems. On the other hand Br2 without additions, caused by an unfavourable equilibrium position gives no measurable LaPO4-transport. Using HBr as transport agent, the transport rate is small. In addition there are difficulties, caused by the partial decomposition of HBr into the elements and the diffusion of H2 through the wall of the quartz ampoule. LaPO4-crystals prepared by chemical transport have the well known monoclinic monazite structure.  相似文献   

3.
Chemical Transport of FeP2 and FeP4 with Iodine Experiments on the chemical transport of FeP2 and FeP4 with iodine are discussed, considering the gaseous molecules I1, I2, FeI2, Fe2I4, FeI3, Fe2I6, PI3, P2I4, P4, P2, and P. Thermodynamic calculations give δH°(298) = 56.322 kcal and ΔS°(298) = 39.5 cal/K for the reaction FeP2,f + I2 = FeI2 + 0.5 P4 and δG°(923) = 35.8 kcal for the reaction FeP4,f + I2 = FeI2 + P4.  相似文献   

4.
The Chemical Transport of Platinum with Chlorine Experiments show that the chemical transport of platinum by means of chlorine within a temperature gradient at temperatures below ≈ 1000°K goes into the hot temperature region, but at higher temperatures in the reverse direction. From the thermodynamic discussion it can be seen, that the platinum content of the gas phase at low temperatures is governed by the exothermic formation of Pt6Cl12,g, and at higher temperatures by the endothermic formation of PtCl3,g and PtCl2,g. The platinum content of the gas phase passes a minimum at ≈ 1000°K, if P(Cl2) = 3.5 atm. This result is in agreement with the observed inversion of the transport direction.  相似文献   

5.
Chemical Vapor Transport of Intermetallic Systems. 9 Chemical Transport of Copper Germanides and Copper Silicides By means of chemical vapor transport using iodine and bromine as transport agents in the system Cu/Ge the compounds Cu3Ge (ϵ and ϵ1), Cu5Ge (ζ) and copper‐rich mixed crystals Cu(Ge) have been prepared in form of single crystals. Thermodynamic considerations allow to understand the CVT process, especially the unexpected low temperatures. Copper silicides can be prepared under similiar conditions. They are extremely disordered. Their crystallographic characterisation was therefore impossible.  相似文献   

6.
The Chemical Transport of the CoS phase The CoSx Phase can be deposited as single crystals by CTR using iodine, only if x is greater than 1.06. This is due to the sulphur phase equilibrium pressure which otherwise is too small for effecting this transport. HI or GeI2 can be used as transport agent for specimens with less sulphur contents. Using GeI2 CTR also yields monocrystals of the Co9S8 phase.  相似文献   

7.
Chemical Vapor Transport of Intermetallic Systems Chemical Transport of Cu/Ag-mixed Crystals By means of chemical transport reaction it is possible to prepare Cu-rich and Ag-rich mixed crystals in the Cu/Ag system. The composition of individual deposited crystals was different. Mass-spectrometric analysis of the gas-phase above CuI/AgI has shown the formation of CuAg2I3,g und Cu2AgI3,g. Thermodynamic computations explain the formation of crystals as well as the reaction conditions.  相似文献   

8.
Chemical Vapor Transport of Intermetallic Systems. Chemical Transport of Co5Ge3 and CoGe By means of transport reaction (900 → 700°C, Iodine as transport agent) pure Co5Ge3 or Co5Ge3 with CoGe as a by-product can be prepared. Thermodynamic calculations allow to understand the reaction semiquantitatively.  相似文献   

9.
The Chemical Transport of Sb2S3 With I2 The chemical transport of Sb2S3 with iodine is discussed on thermodynamical basis under consideration of the gaseous molecules I2, I1, SbI3, S2, S3, S4, S5, S6, S7 and S8. The experiments are in a satisfying agreement with the calculations.  相似文献   

10.
Chemical Vapor Transport of Intermetallic Systems. 2. Chemical Transport of Co/Ni-mixed Crystals By means of chemical transport reaction it is possible to prepare Co/Ni-mixed crystals in a wide range of percentage composition between 5 and 75 weight % Nickel. This is possible using a 3-zone-oven. Thermodynamic considerations allow to understand the experiments.  相似文献   

11.
The Chemical Transport of Silver with Iodine and the Inversion of the Transport Direction in the Temperature-Gradient The formation of Ag3I3,g from Ag,s and I,g is exothermic, the corresponding formation of AgI,g is endothermic. Depending on the temperature one expects chemical transport of Ag into the higher or the lower temperature region. This inversion of the transport direction has been calculated thermodynamically and experimentally observed.  相似文献   

12.
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   

13.
Chemical Vapor Transport of Intermetallic Systems. 3. Chemical Transport of Mo/W-mixed Crystals Mo/W-mixed crystals can be prepared by means of chemical vapor transport with HgBr2 (1000°C→900°C). It is known [2] that the transport reaction of tungsten begins hours or even days after starting the experiment. This is the reason for the unusual composition of deposited crystals: EDX-analysis show them to have a Mo-rich nucleus and a W-rich shell.  相似文献   

14.
Mass Spectrum of the System Te/S and the Chemical Transport of Tellurium with Sulphur The mixed molecules TeSx (x = 1 … 7) and Te2Sy (y = 1 … 6) have been observed by mass spectrometry. These molecules are responsible for the fact, that Tellurium can be chemically transported by means of sulphur in a temperature gradient (375 → 325°C).  相似文献   

15.
Chemical Vapor Transport of Intermetallic Systems. 5. Chemical Transport of Ni3Sn and Ni3Sn2 The congruent melting intermetallic compounds. Ni3Sn and Ni3Sn2 can be prepared by CVT-methods using Iodine as transport agent. Thermodynamic calculations allow to understand why Ni3Sn and Ni3Sn2 but not Ni3Sn4 can be prepared by this manner. Some general rules concerning CVT of intermetallics are given.  相似文献   

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17.
Studies on the Chemical Transport of Nickel with Carbon Monoxide in a Sealed Reaction Space The chemical transport of nickel by means of carbon monoxide (equation (1)) has been investigated experimentally in closed ampoules of a special shape. Besides the experiments the transport rate has been calculated approximately for different models assuming equilibrium between solid and gas motion by diffusion and stoichiometric flow. It is shown that the transport rate calculated in this way (with one exception) is between the limits given by calculation for diffusion only and neglecting the stoichiometric flow. The equilibrium pressures calculated with ΔH°1(298) = ?35.0 kcal lead to transport rates which agree approximately with the rate determined experimentally (c. f. Table 4).  相似文献   

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