HEATED BODY-TEMPERATURE MEASUREMENT BY SPECTROMETRY OF PHOTOELECTRONS

Authors
Citation
Kn. Kasparov, HEATED BODY-TEMPERATURE MEASUREMENT BY SPECTROMETRY OF PHOTOELECTRONS, Measurement science & technology, 9(9), 1998, pp. 1388-1399
Citations number
17
Categorie Soggetti
Instument & Instrumentation",Engineering
ISSN journal
09570233
Volume
9
Issue
9
Year of publication
1998
Pages
1388 - 1399
Database
ISI
SICI code
0957-0233(1998)9:9<1388:HBMBSO>2.0.ZU;2-6
Abstract
It is shown that the heated body temperature can be measured from the energy distribution of photoelectrons appearing in the photoelectric d evice which serves simultaneously as detector and analyser of the body radiation spectrum. The effective wavelengths of this temperature mea suring technique cannot be chosen arbitrarily because they are functio ns of the temperature and must be measured. A technique for measuring the series of values of the effective wavelengths lambda(r)(T), which is necessary for estimation of the procedural error Delta T-ph, has be en proposed. The latter depends on the type of spectral characteristic of the photodetector, the energy photoelectron dispersion D in a reta rding field and the emissivity of a heated surface epsilon(lambda, T). The formulae for the procedural error calculation are obtained and th e latter has been shown to be less than that for measuring the tempera ture by conventional optical pyrometry methods and almost independent of temperature; Delta T-ph approximate to 2-3 K for tungsten (when T = 1200-2600 K) and Delta T-ph approximate to 3-5 K for platinum (when T = 1200-1800 K). The calculated results have been proved by series of experiments. A photoemissive pyrometer based on this method can be emp loyed for temperature measurements when the exact meaning of a changea ble emissivity is unknown as it takes place, for example, at pulse hea ting processes.