The possibility of simplified modelling of radiation heat transfer within a steel porous charge
R Wyczółkowski, T Wyleciał… - MATEC Web of …, 2018 - matec-conferences.org
R Wyczółkowski, T Wyleciał, M Gała
MATEC Web of Conferences, 2018•matec-conferences.orgThe article refers to the problem of calculating the effective thermal conductivity k ef of a steel
porous charge. In proposed approach for each heat transfer mechanism, which occurs in the
considered medium, the corresponding thermal resistance is assigned. The model values of
the k ef coefficient were determined twice for the same input data (geometric dimensions,
emissivity, temperature, thermal conductivity of steel and gas). The difference between
successive calculations depended on the use of two different methods to determine the …
porous charge. In proposed approach for each heat transfer mechanism, which occurs in the
considered medium, the corresponding thermal resistance is assigned. The model values of
the k ef coefficient were determined twice for the same input data (geometric dimensions,
emissivity, temperature, thermal conductivity of steel and gas). The difference between
successive calculations depended on the use of two different methods to determine the …
The article refers to the problem of calculating the effective thermal conductivity kef of a steel porous charge. In proposed approach for each heat transfer mechanism, which occurs in the considered medium, the corresponding thermal resistance is assigned. The model values of the kef coefficient were determined twice for the same input data (geometric dimensions, emissivity, temperature, thermal conductivity of steel and gas). The difference between successive calculations depended on the use of two different methods to determine the thermal radiation resistance Rrd. In the first approach the resistance Rrd was calculated using the exact method and in the second approach the simplified, approximate method was used. The discrepancy between the obtained results of kef in both approaches provides the evidence to use the approximate method to determine the resistance Rrd. A bundle of square steel sections were used to demonstrate the challenge. In the exact method, data regarding the temperature distribution within a single profile was used. These data were obtained based on experimental research using a guarded hot plate apparatus. The calculations were performed using a temperature range between 200ºC and 800ºC for two sections: 60×60mm and 80×80mm and three emissivities: 0.5, 0.7 and 0.9.
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