scholarly journals Simultaneous measurements of heat capacity, electrical resistivity and hemispherical total emittance by a pulse heating technique: zirconium, 1500 to 2100 K

1974 ◽  
Vol 78A (4) ◽  
pp. 509 ◽  
Author(s):  
A. Cezairliyan ◽  
F. Righini
Keyword(s):  
Heat Capacity ◽  
Electrical Resistivity ◽  
Pulse Heating ◽  
Simultaneous Measurements ◽  
Pulse Heating Technique ◽  
Hemispherical Total Emittance ◽  
Total Emittance

scholarly journals Electrical resistivity measured by millisecond pulse-heating in comparison to thermal conductivity of the hot work tool steel AISI H11 (1.2343) at elevated temperature

2020 ◽  
Vol 49 (1-2) ◽  
pp. 75-87
Author(s):  
ERHARD KASCHNITZ ◽  
PETER HOFER-HAUSER ◽  
WALTER FUNK
Keyword(s):  
Thermal Conductivity ◽  
Differential Scanning Calorimetry ◽  
Heat Capacity ◽  
Electrical Resistivity ◽  
Tool Steel ◽  
Room Temperature ◽  
Pulse Heating ◽  
Scanning Calorimetry ◽  
Hot Work Tool Steel ◽  
Steel Aisi

Selected thermophysical properties of the hot work tool steel AISI H11 (1.2343) were measured in the temperature range from room temperature to the melting temperature. Thermal diffusivity was measured by the laser-flash method; heat capacity by differential scanning calorimetry; linear thermal expansion by push-rod dilatometry; and density at room temperature by an Archimedean balance. From these experimentally obtained data, thermal conductivity was calculated. Additionally, electrical resistivity of AISI H11 (1.2343) was measured by millisecond pulse-heating in the above mentioned temperature range. The measurement results of electrical resistivity as a function of specific enthalpy was combined with results of specific heat capacity measurements by differential-scanning calorimetry to obtain the relation between resistivity and temperature. Based on measured electrical resistivity and thermal conductivity, a Smith-Palmer-plot for the hot work tool steel AISI H11 (1.2343) is obtained for the ferritic and austenitic phases. No linear behaviour – as expected by the Wiedemann-Franz law – is observed in the ferritic phase region. In the high temperature austenitic region, the thermal conductivity can be computed from electrical resistivity using empirical constants of similar austenitic steels or superalloys.

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