statisticalgeofluidmechanics blogspot.com

Statistical Geofluid Mechanics

Saturday, February 16, 2008. Case of the metal bar revised version. The case of the metal bar is revised from this post. The main error made in these previous posts is that the the heat flux q. Was chosen proportional to . T instead of . 1T according to the phenomenological law. Thus, the profile corresponding to the minimum entropy principle did not correspond to the profile of a steady state . The linear profile we learnt is only an approximation of the real steady state profile. Constant in x t.

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Statistical Geofluid Mechanics

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Saturday, February 16, 2008. Case of the metal bar revised version. The case of the metal bar is revised from this post. The main error made in these previous posts is that the the heat flux q. Was chosen proportional to . T instead of . 1T according to the phenomenological law. Thus, the profile corresponding to the minimum entropy principle did not correspond to the profile of a steady state . The linear profile we learnt is only an approximation of the real steady state profile. Constant in x t.

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This web page statisticalgeofluidmechanics.blogspot.com states the following, "Saturday, February 16, 2008." We saw that the webpage said " Case of the metal bar revised version." It also said " The case of the metal bar is revised from this post. The main error made in these previous posts is that the the heat flux q. Was chosen proportional to . 1T according to the phenomenological law. Thus, the profile corresponding to the minimum entropy principle did not correspond to the profile of a steady state . The linear profile we learnt is only an approximation of the real steady state profile."

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