|
Teplofizika vysokikh temperatur, 1991, Volume 29, Issue 3, Pages 474–479
(Mi tvt4238)
|
|
|
|
Thermophysical Properties of Materials
Thermodynamics of gaseous zirconium and hafnium fluorides
N. V. Barkovskiiab, V. I. Tsirel'nikovba, A. M. Emel'yanovab, Yu. S. Khodeevba a Moscow State (V. I. Lenin) Pedagogical Institute
b Institute for High Temperatures, USSR Academy of Sciences
Abstract:
An MS 1301 magnetic mass spectrometer has been used over a wide temperature range to examine vapor-state equilibria involving zirconium and hafnium fluorides. The enthalpies of formation have been determined for all the lower fluorides of those elements. These results are new for zirconium and hafnium monofluorides and also for hafnium difluoride and trifluoride. The recommended values are $\Delta_fH^0(\mathrm{HfF}_3, g, 0) = -1075 \pm 13, \Delta_fH^0(\mathrm{ZrF}_3, g, 0) = -1078 \pm 15, \Delta_fH^0(\mathrm{HfF}_2, g, 0) = -512 \pm 12, \Delta_fH^0(\mathrm{ZrF}_2, g, 0) = -483 \pm 16, \Delta_fH^0(\mathrm{HfF}, g, 0) = 53 \pm 12, \Delta_fH^0(\mathrm{ZrF}, g, 0) = 63 \pm 12$ kJ $\cdot$ mole$^{-1}$. The measurements have been used to calculate the equilibrium vapor compositions and the bond energies. The recommended values are $D^0(0), n$: $D^0(\mathrm{ZrF}_3$–$\mathrm{F}) = 665 \pm 15, D^0(\mathrm{ZrF}_2$–$\mathrm{F}) = 672 \pm 18, D^0(\mathrm{ZrF}$–$\mathrm{F}) = 623 \pm 16, D^0(\mathrm{Zr}$–$\mathrm{F}) = 612 \pm 15, D^0(\mathrm{HfF}_3$–$\mathrm{F}) = 702 \pm 18, D^0(\mathrm{HfF}_2$–$\mathrm{F}) = 640 \pm 20, D^0(\mathrm{HfF}$–$\mathrm{F}) = 642 \pm 14, D^0(\mathrm{Hf}$–$\mathrm{F}) = 646 \pm 15$, kJ $\cdot$ mole$^{-1}$.
Received: 11.12.1989
Citation:
N. V. Barkovskii, V. I. Tsirel'nikov, A. M. Emel'yanov, Yu. S. Khodeev, “Thermodynamics of gaseous zirconium and hafnium fluorides”, TVT, 29:3 (1991), 474–479; High Temperature, 29:3 (1991), 371–375
Linking options:
https://www.mathnet.ru/eng/tvt4238 https://www.mathnet.ru/eng/tvt/v29/i3/p474
|
|