2002
DOI: 10.1021/je010254f
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Vapor Pressure and Sublimation Enthalpies of Holmium Trichloride, Tribromide, and Triiodide

Abstract: The total vapor pressure of HoCl 3 , HoBr 3 , and HoI 3 was measured by the torsion and Knudsen effusion methods. By a least-squares treatment of the obtained data, the following equations were selected as representative for the temperature dependence of their vapor pressures in the covered temperature ranges: HoCl 3 (s), log(p/kPa) ) 10.91 ( 0.10 -(14216 ( 150) (K/T) (from 883 to 994 K); HoCl 3 (1), log(p/ kPa) ) 9.16 ( 0.10 -(12466 ( 150) (K/T) (from 1002 to 1164 K); HoBr 3 (s) log(p/kPa) ) 10.95 ( 0.10 -(14… Show more

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Cited by 21 publications
(15 citation statements)
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“…This average value agrees with that selected by Gietmann et al, , (288.2 ± 6.1) kJ·mol -1 , obtained from the second-law, (293 ± 7) kJ·mol -1 , and third-law, (279 ± 10) kJ·mol -1 , values. Our selected value seems to be decidedly comparable with those obtained by us for tribromides of other heavy lanthanides: GdBr 3 = (292 ± 2), TbBr 3 = (287 ± 4), DyBr 3 = (289 ± 6), and HoBr 3 = (290 ± 5) kJ·mol -1 7 Comparison of the free energy function for solid lanthanide triiodides reported by Pankratz: 19 (▪) LaI 3 ; (○) CeI 3 ; (·) PrI 3 ; (▵) NdI 3 ; (▴) GdI 3 ; (×) TbI 3 ; (□) HoI 3 (Piacente et al); (◇) ErI 3 (this work). 6 Free Energy Function for Solid ErI 3 Calculated by the Third-Law Method, Δ s ub H °(298 K) = (282 ± 6) kJ·mol -1 ( p ° = 1 atm = 101.325 kPa) − R ln( p /atm)−Δfef−fef(g) a −fef(s) T p KkPaJ·K -1 · mol -1 J·K -1 · mol -1 J·K -1 · mol -1 J·K -1 · mol -1 900 1.40 × 10 -4 112.2 201 467.4 266 950 9.05 × 10 -4 96.6 200 470.4 270 1000 4.86 × 10 -3 82.7 200 473.3 273 1050 2.22 × 10 -2 70.0 199 476.2 277 1100 8.84 × 10 -2 58.6 198 479.0 281 a Selected by Pankratz
…”
Section: Discussionsupporting
confidence: 80%
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“…This average value agrees with that selected by Gietmann et al, , (288.2 ± 6.1) kJ·mol -1 , obtained from the second-law, (293 ± 7) kJ·mol -1 , and third-law, (279 ± 10) kJ·mol -1 , values. Our selected value seems to be decidedly comparable with those obtained by us for tribromides of other heavy lanthanides: GdBr 3 = (292 ± 2), TbBr 3 = (287 ± 4), DyBr 3 = (289 ± 6), and HoBr 3 = (290 ± 5) kJ·mol -1 7 Comparison of the free energy function for solid lanthanide triiodides reported by Pankratz: 19 (▪) LaI 3 ; (○) CeI 3 ; (·) PrI 3 ; (▵) NdI 3 ; (▴) GdI 3 ; (×) TbI 3 ; (□) HoI 3 (Piacente et al); (◇) ErI 3 (this work). 6 Free Energy Function for Solid ErI 3 Calculated by the Third-Law Method, Δ s ub H °(298 K) = (282 ± 6) kJ·mol -1 ( p ° = 1 atm = 101.325 kPa) − R ln( p /atm)−Δfef−fef(g) a −fef(s) T p KkPaJ·K -1 · mol -1 J·K -1 · mol -1 J·K -1 · mol -1 J·K -1 · mol -1 900 1.40 × 10 -4 112.2 201 467.4 266 950 9.05 × 10 -4 96.6 200 470.4 270 1000 4.86 × 10 -3 82.7 200 473.3 273 1050 2.22 × 10 -2 70.0 199 476.2 277 1100 8.84 × 10 -2 58.6 198 479.0 281 a Selected by Pankratz
…”
Section: Discussionsupporting
confidence: 80%
“…Comparison of the free energy function for solid lanthanide triiodides reported by Pankratz: 19 (▪) LaI 3 ; (○) CeI 3 ; (·) PrI 3 ; (▵) NdI 3 ; (▴) GdI 3 ; (×) TbI 3 ; (□) HoI 3 (Piacente et al); (◇) ErI 3 (this work).…”
Section: Discussionmentioning
confidence: 71%
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“…5 The mass spectrum of the vapor over TmI 3 was determined at 913 K, 6 and this was very similar to those of other triiodides of the rare-earth elements. 7 This work is part of a continuing systematic study [8][9][10][11][12][13][14][15][16] carried out in order to obtain accurate measurements of the vapor pressures of rare-earth trihalides and to derive their standard sublimation enthalpies. In particular, the aim of the present paper was to determine the standard sublimation enthalpies of thulium trichloride, tribromide, and triiodide measuring their vapor pressures.…”
Section: Introductionmentioning
confidence: 99%