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.