Thermal Conductivity of Grade UPV-1 Pyrolytic Graphite at 1900–2950 K
The need to account for a misalignment between the heat flux density and temperature gradient vectors when studying thermal conductivity of anisotropic materials was analyzed. A method for measuring thermal conductivity of pyrolytic graphite (grade UPV-1) in the direction parallel to the precipitati...
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Published in | Measurement techniques Vol. 63; no. 9; pp. 736 - 740 |
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Main Authors | , , , |
Format | Journal Article |
Language | English |
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01.12.2020
Springer Springer Nature B.V |
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Abstract | The need to account for a misalignment between the heat flux density and temperature gradient vectors when studying thermal conductivity of anisotropic materials was analyzed. A method for measuring thermal conductivity of pyrolytic graphite (grade UPV-1) in the direction parallel to the precipitation plane was proposed. The advantage of the proposed method is the possibility to determine thermal conductivity of pyrolytic graphite in the direction parallel to the precipitation plane while accounting for a misalignment between the heat flux density and temperature gradient vectors. The test samples were shaped as hollow cylinders with the pyrolytic graphite precipitation plane located along the radius of the cylinder. The heat flux density was determined based on the radiation heat flux emitted from the outer surface of the sample, and the temperature gradient was calculated along the radius, which made it possible to maintain the alignment between the heat flux density and temperature gradient vectors. A comparative analysis of the thermal conductivity values obtained in this study (parallel to the precipitation plane) and those reported in the reference sources was performed. The studied temperature range was extended into the higher temperature region by 450 K and constitutes 1900–2950 K. |
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AbstractList | The need to account for a misalignment between the heat flux density and temperature gradient vectors when studying thermal conductivity of anisotropic materials was analyzed. A method for measuring thermal conductivity of pyrolytic graphite (grade UPV-1) in the direction parallel to the precipitation plane was proposed. The advantage of the proposed method is the possibility to determine thermal conductivity of pyrolytic graphite in the direction parallel to the precipitation plane while accounting for a misalignment between the heat flux density and temperature gradient vectors. The test samples were shaped as hollow cylinders with the pyrolytic graphite precipitation plane located along the radius of the cylinder. The heat flux density was determined based on the radiation heat flux emitted from the outer surface of the sample, and the temperature gradient was calculated along the radius, which made it possible to maintain the alignment between the heat flux density and temperature gradient vectors. A comparative analysis of the thermal conductivity values obtained in this study (parallel to the precipitation plane) and those reported in the reference sources was performed. The studied temperature range was extended into the higher temperature region by 450 K and constitutes 1900-2950 K. |
Audience | Academic |
Author | Kostanovskiy, А. V. Pronkin, A. A. Zeodinov, M. G. Kostanovskaya, M. E. |
Author_xml | – sequence: 1 givenname: А. V. surname: Kostanovskiy fullname: Kostanovskiy, А. V. email: Kostanovskiy@gmail.com, laimfam@gmail.com organization: Joint Institute of High Temperatures, Russian Academy of Sciences (JIHT RAS) – sequence: 2 givenname: M. E. surname: Kostanovskaya fullname: Kostanovskaya, M. E. organization: Joint Institute of High Temperatures, Russian Academy of Sciences (JIHT RAS) – sequence: 3 givenname: M. G. surname: Zeodinov fullname: Zeodinov, M. G. organization: Joint Institute of High Temperatures, Russian Academy of Sciences (JIHT RAS) – sequence: 4 givenname: A. A. surname: Pronkin fullname: Pronkin, A. A. organization: Joint Institute of High Temperatures, Russian Academy of Sciences (JIHT RAS) |
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Cites_doi | 10.1016/j.applthermaleng.2010.04.014 |
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Keywords | temperature gradient vector pyrolytic graphite thermal conductivity heat flux density vector |
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References | WangLWTamainot-TeltoZMetcalfSJAppl. Therm. Eng.201030131805181110.1016/j.applthermaleng.2010.04.014 SosedovVPProperties of Carbon-based Construction Materials1975MoscowMetallurgiya KostanovskiiAVZeodinovMGKostanovskayaMEThermal conductivity and emissivity of DE-24 graphite at 2300–3000 KIzmer. Tekhn.2010123841 A. V. Kostanovskii, M. G. Zeodinov, M. E. Kostanovskaya, and A. A. Pronkin, “Thermal conductivity of silicified silicon carbide at 1400–2200 K,” Teplofi z. Vys. Temp., 57, No. 1, 137–139 (2019), https://doi.org/101134S0040364419010150. L. N. Latyev, V. A. Petrov, V. Ya. Chekhovskoi, and E. N. Shestakov, Radiation Properties of Solid Materials. Reference Book, A. E. Sheindlin (ed.), Energiya, Moscow (1974). MiszczakMŚwiderskiWInt. J. Mod. Manuf. Technol.2012425560 ChekhovskoiVYPetrovVAPetrovaIILukshinENTeplofi z. Vys. Temp.1971918084 KostanovskiiAVKostanovskayaMEZeodinovMGOn phonon mechanism of thermal conductivity of graphite at high temperaturesTeplofi z. Vys. Temp.2013513477480 С. Y. Ho, R. W. Powell, and P. E. Liley, Thermal Conductivity of Selected Materials. Pt. 2, SupDocs GPO, Washington (1968). PrigozhinIKondepudiDThermodynamicsMFrom Heat Engines to Dissipative Structures [Russian translation]2002MoscowMir 1847_CR8 AV Kostanovskii (1847_CR9) 2010; 12 LW Wang (1847_CR1) 2010; 30 AV Kostanovskii (1847_CR3) 2013; 51 1847_CR5 M Miszczak (1847_CR2) 2012; 4 1847_CR10 VY Chekhovskoi (1847_CR6) 1971; 9 VP Sosedov (1847_CR4) 1975 I Prigozhin (1847_CR7) 2002 |
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SubjectTerms | Analytical Chemistry Anisotropy Characterization and Evaluation of Materials Flux density Graphite Heat conductivity Heat flux Heat transfer Herbivores Measurement methods Measurement Science and Instrumentation Misalignment Physical Chemistry Physics Physics and Astronomy Pyrolytic graphite Thermal conductivity Thermophysical Measurements |
Title | Thermal Conductivity of Grade UPV-1 Pyrolytic Graphite at 1900–2950 K |
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