B. T. Barnes
Total radiation data were obtained on polished nickel and on the same metal when covered with soot. Temperatures below the range of an optical pyrometer were determined from a log-resistance vs log-temperature curve obtained from resistance measurements on the wire mounted in a lamp in a furnace at known temperatures and extended up to the points obtained when using a pyrometer. The log-resistance vs log-temperature curve had a sharp break at the magnetic transformation point just as noted by previous investigators. This break occurred at about 360°C. In the region from 800 to 900° the total radiation values for unpolished nickel deviated somewhat from a smooth curve through the values at lower and higher temperatures. This may be due to an error in drawing the log-resistance vs log-temperature curve since there were no resistance temperature measurements from 500 to 725°C between the range of the furnace readings and that of the pyrometer. Total emissivity values for soot-covered nickel range from 0.92 at 400°K to a mimimum value of 0.81 at 800°K, then rise to 0.86 at 1100A°K. The total emissivity of polished nickel was found to be 0.205 at 1400°K. At 400°K it was 0.087 before heating to incandescence and 0.063 afterwards. At intermediate temperatures there were similar differences due to surface changes during the initial heating. © 1929 The American Physical Society.
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