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翻訳と辞書　辞書検索 [ 開発暫定版 ] スポンサード リンク Second-order fluid ： ウィキペディア英語版 Second-order fluid A second-order fluid is a fluid where the stress tensor is the sum of all tensors that can be formed from the velocity field with up to two derivatives. So that the total stress tensor can be written :$$ \tau = -p 1 + C_1 A + C_2 A^2 + C_3 A_u + C_4 A_l, where $A$ is the strain tensor, $A\_u$ is the upper convected derivative of $A$ and $A\_l$ is the lower convected derivative of $A$. The coefficients $C\_i$ are functions of the tensor invariants of $A$. An Euler fluid is a zeroth order fluid and a Newtonian fluid is a first order one. For a steady flow this can be written :$$ \tau = -p 1 + C_1 A + C_2 A^2 + C_5 B, where B is the second Rivlin-Ericksen tensor, and $C\_5$ is a new constant. ==References== Bird, RB., Armstrong, RC., Hassager, O., Dynamics of Polymeric Liquids: Second Edition, Volume 1: Fluid Mechanics. John Wiley and Sons 1987 ISBN 047180245X(v.1) Bird R.B, Stewart W.E, Light Foot E.N.: Transport phenomena, John Wiley and Sons, Inc. New York, U.S.A., 1960 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Second-order fluid」の詳細全文を読む スポンサード リンク 翻訳と辞書 : 翻訳のためのインターネットリソース Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.