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Titlebook: Rough Sets and Current Trends in Computing; 4th International Co Shusaku Tsumoto,Roman S?owiński,Jerzy W. Grzyma?a- Conference proceedings

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發(fā)表于 2025-3-23 11:46:17 | 只看該作者
Tetsuya Murai,Masayuki Sanada,Y. Kudo,Mineichi Kudo
12#
發(fā)表于 2025-3-23 15:09:07 | 只看該作者
Aida Vitória,Carlos Viegas Damásio,Jan Ma?uszyński
13#
發(fā)表于 2025-3-23 20:39:05 | 只看該作者
14#
發(fā)表于 2025-3-24 00:27:56 | 只看該作者
15#
發(fā)表于 2025-3-24 03:40:56 | 只看該作者
Zdzis?aw Pawlakvity of a “bulk” material (that is, a large sample that is by definition free of microscale effects) to the effective thermal conductivity of a microscopic sample of the same material. The values of thermal conductivity that are readily available in textbooks and standard reference books (so-called
16#
發(fā)表于 2025-3-24 09:04:28 | 只看該作者
Lech Polkowskivity of a “bulk” material (that is, a large sample that is by definition free of microscale effects) to the effective thermal conductivity of a microscopic sample of the same material. The values of thermal conductivity that are readily available in textbooks and standard reference books (so-called
17#
發(fā)表于 2025-3-24 12:41:51 | 只看該作者
Masahiro Inuiguchinsfer in living tissue, numerical solutions using MATLAB?, and microscale conduction. This makes the book unique among the many published textbooks on conduction heat transfer. Other noteworthy features of the book are:?.The material is organized to provide students with the tools to model, analyze,
18#
發(fā)表于 2025-3-24 16:35:27 | 只看該作者
Gianpiero Cattaneo,Davide Ciuccincludes numerical modelling of heat conductionThis textbook presents the classical topics of conduction heat transfer and extends the coverage to include chapters on perturbation methods, heat transfer in living tissue, numerical solutions using MATLAB?, and microscale conduction. This makes the boo
19#
發(fā)表于 2025-3-24 21:22:57 | 只看該作者
20#
發(fā)表于 2025-3-25 01:08:24 | 只看該作者
Yiyu YaoOURIER‘s ideas and methods at the hands of many authors, provide a highly successful theory of heat conduction. According to that theory, the growth or decay of the temperature e in a conducting body is governed by the heat equation, that is, by the parabolic partial differential equation Such has b
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