Article
Thermophysical Properties of Materials
2008. V. 46. № 3. P. 350–356
Kudin L.S., Butman M.F., Motalov V.B., Grishin A.E., Kryuchkov A.S., Bergman G.A.
The thermodynamic parameters of monomer and dimer molecules of cerium and praseodymium tribromides
Annotation
The method of high-temperature mass spectrometry is used for studying the composition of saturated vapor over cerium and praseodymium tribromides. Monomer and dimer molecules are found in the temperature ranges of 789–994 K and 804–957 K for cerium and praseodymium, respectively. The partial pressures of vapor components are determined, p(Pa), the temperature dependences of which are approximated by the equations logp(CeBr3)=(−14.63±0.08)×103/T+(14.54±0.09),T=789−994 K;logp(Ce2Br6)=(−19.72±0.61)×103/T+(17.60±0.64),T=918−980 K;logp(PrBr3)=(−14.13±0.12)×103/T+(14.09±0.14),T=804−957 K;logp(Pr2Br6)=(−18.90±0.50)×103/T+(17.15±0.53),T=903−955 K. The values of pressure of vapor components are used along with literature data for the calculation of enthalpies of sublimation in the form of monomer and dimer molecules by the procedures of the second and third laws of thermodynamics. Based on analysis of the results, thermodynamic parameters of monomer and dimer molecules (in kJ mol−1) are recommended, ΔsH0(CeBr3,298.15)=305±5,ΔsH0(PrBr3,298.15)=293±5,ΔsH0(Ce2Br6,298.15)=410±28,ΔsH0(Pr2Br6,298.15)=403±28,ΔfH0(CeBr3,gas,298.15)=−587±6,ΔfH0(PrBr3,gas,298.15)=−597±7,ΔfH0(Ce2Br6,gas,298.15)=−1372±28,ΔfH0(Pr2Br6,gas,298.15)=−1378±28.
Article reference:
Kudin L.S., Butman M.F., Motalov V.B., Grishin A.E., Kryuchkov A.S., Bergman G.A. The thermodynamic parameters of monomer and dimer molecules of cerium and praseodymium tribromides, High Temp., 2008. V. 46. № 3. P. 350
Kudin L.S., Butman M.F., Motalov V.B., Grishin A.E., Kryuchkov A.S., Bergman G.A. The thermodynamic parameters of monomer and dimer molecules of cerium and praseodymium tribromides, High Temp., 2008. V. 46. № 3. P. 350