A COMBINED TRANSIENT AND BRIEF STEADY-STATE TECHNIQUE FOR MEASURING HEMISPHERICAL TOTAL EMISSIVITY OF ELECTRICAL CONDUCTORS AT HIGH-TEMPERATURES - APPLICATION TO TANTALUM
T. Matsumoto et A. Cezairliyan, A COMBINED TRANSIENT AND BRIEF STEADY-STATE TECHNIQUE FOR MEASURING HEMISPHERICAL TOTAL EMISSIVITY OF ELECTRICAL CONDUCTORS AT HIGH-TEMPERATURES - APPLICATION TO TANTALUM, International journal of thermophysics, 18(6), 1997, pp. 1539-1556
A new method for measuring hemispherical total emissivity of electrica
lly conducting materials at high temperatures (above 1500 K) using a f
eedback-controlled pulse-heating technique has been developed. The tec
hnique is based on rapid resistive self-heating of a solid cylindrical
specimen in vacuum up to a preset high temperature in a short time (a
bout 200 ms) and then keeping the specimen at that temperature under s
teady state conditions for a brief period (about 500 ms) before switch
ing off the current through the specimen. The specimen is maintained a
t constant temperature with a feedback control system which controls t
he current through the specimen. The computer-controlled feedback syst
em operates a solid-state switch (composed of field-effect transistors
). The sensing signal for the feedback is provided by a high-speed opt
ical pyrometer. Hemispherical total emissivity is determined at the te
mperature plateau from the data on current through the specimen, the v
oltage drop across the middle portion of the specimen, and the specime
n temperature using the steady-state heat balance equation based on th
e Stefan-Boltzmann law. The true temperature of the specimen is determ
ined from the measured radiance temperature and the normal spectral em
issivity; the latter is obtained from laser polarimetric measurements.
The experimental quantities are measured and recorded every 0.2 ms wi
th a 12-bit digital oscilloscope. To demonstrate the feasibility of th
e technique, experiments were conducted on a tantalum specimen in the
temperature range 2000 to 2800 K. The results on hemispherical total e
missivity are presented and are compared with the data given in the li
terature.