Аннотации:
When measuring the thermal conductivity of thermal insulation materials made by powder
metallurgy and building porous materials, complications arise due to the fact that heat flows
through the samples are commensurate with heat losses. The steady-state heat flow (SSHF)
method is simple, does not require sophisticated equipment, and allows determining the thermal
conductivity not in the near-surface layer but in the entire sample volume. Its disadvantage is low
accuracy and the need to use reference samples.
This work aims to develop an installation for measuring the thermal conductivity of largesized
samples of low-conductivity material using the steady-state heat flow method with significantly
higher accuracy than existing installations using this method.
This is achieved by sandwiching the sample, which is a thin square plate of large dimensions,
between the heater chamber and the refrigerator. The heating chamber is made of insulating
material and its front wall, which is in contact with the sample, is made of the copper
plate (which has good thermal conductivity). In the operating mode, the temperature in
the heater chamber is maintained equal to the ambient temperature, which allows us to
neglect heat losses and assume that in the steady-state mode, the heater power is equal to
the heat flux through the sample. The thickness of the sample is much smaller than the size
of its side (the sample should be square). This assumption is necessary to use the condition
of isotropic temperature distribution in the cross-section of the sample. The refrigerator is
filled with water and ice. The isotropic temperature distribution in the sample is ensured by
its contact with the copper walls of the heater and refrigerator chamber. The temperature
of the heated surface of the sample is measured using a thermocouple inserted through a hole
in the front wall of the heater chamber
The proposed design of the installation and its operating conditions make it possible to significantly
improve the accuracy of determining the thermal conductivity coefficient and make
the error less than 2%.
