Thermophysical properties of zirconium at high temperature

Citation
Pf. Paradis et Wk. Rhim, Thermophysical properties of zirconium at high temperature, J MATER RES, 14(9), 1999, pp. 3713-3719
Citations number
22
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Material Science & Engineering
Journal title
JOURNAL OF MATERIALS RESEARCH
ISSN journal
08842914 → ACNP
Volume
14
Issue
9
Year of publication
1999
Pages
3713 - 3719
Database
ISI
SICI code
0884-2914(199909)14:9<3713:TPOZAH>2.0.ZU;2-G
Abstract
Six thermophysical properties of both solid and liquid zirconium measured u sing the high-temperature electrostatic levitator at the Jet Propulsion Lab oratory are presented. These properties are density, thermal expansion coef ficient, constant pressure heat capacity, hemispherical total emissivity, s urface tension, and viscosity. For the first time, we report the densities and the thermal expansion coefficients of both the solid as well as liquid Zr over wide ranges of temperatures. Over the 1700-2300 K temperature span, the liquid density can be expressed as rho(1)(T) = 6.24 x 10(3) - 0.29(T - T-m) kg/m(3) with T-m = 2128 K, and the corresponding volume expansion coe fficient as alpha(1) = 4.6 x 10(-5) /K. Similarly, over the 1250-2100 K ran ge, the measured density of the solid can be expressed as rho(s)(T) = 6.34 x 10(3) - 0.15(T - T-m), giving a volume expansion coefficient alpha(s) = 2 .35 x 10(-5) /K. The constant pressure heat capacity of the liquid phase co uld be estimated as C-pl(T) = 39.72 - 7.42 x 10(-3) (T - T-m) J/(mol/K) if the hemispherical total emissivity of the liquid phase epsilon(T1) remains constant at 0.3 over the 1825-2200 K range. Over the 1400-2100 K temperatur e span, the hemispherical total emissivity of the solid phase could be rend ered as epsilon(Ts)(T) = 0.29 - 9.91 x 10(3) (T - T-m). The measured surfac e tension and the viscosity of the molten zirconium over the 1850-2200 K ra nge can be expressed as sigma(T) = 1.459 x 10(3) - 0.244 (T - T-m) mN/m and as eta(T) = 4.83 - 5.31 x 10(-3)(T - T-m) mPa s, respectively.