{"title":"Addendum to: “Dynamics of incompressible fluids with incompatible distortion rates” [International Journal of Engineering Science 168C (2021)]","authors":"Roger Fosdick , Eliot Fried","doi":"10.1016/j.ijengsci.2024.104162","DOIUrl":null,"url":null,"abstract":"<div><div>Fosdick and Fried (2021) proposed a generalized Navier–Stokes theory for studying the dynamics of incompressible fluids which, under certain flow conditions, may support incompatible distortion rates. Herein, we complete the development of a comprehensive boundary condition, at a fixed wall, for the incompatibility tensor <span><math><mi>G</mi></math></span> of that theory; we clarify the physical conditions which express the presence of incompatibility at a wall and, thus, its transmission into the adjacent fluid. The final condition incorporates a constitutively prescribed threshold <span><math><msub><mrow><mi>τ</mi></mrow><mrow><mi>c</mi></mrow></msub></math></span> for the magnitude of the shear stress vector <span><math><mi>s</mi></math></span> at the wall. For <span><math><mrow><mrow><mo>|</mo><mi>s</mi><mo>|</mo></mrow><mo><</mo><msub><mrow><mi>τ</mi></mrow><mrow><mi>c</mi></mrow></msub></mrow></math></span>, <span><math><mrow><mi>G</mi><mo>=</mo><mi>O</mi></mrow></math></span>. For <span><math><mrow><mrow><mo>|</mo><mi>s</mi><mo>|</mo></mrow><mo>≥</mo><msub><mrow><mi>τ</mi></mrow><mrow><mi>c</mi></mrow></msub></mrow></math></span>, <span><math><mrow><mi>G</mi><mo>=</mo><mi>γ</mi><mrow><mo>(</mo><mi>1</mi><mo>−</mo><mi>t</mi><mo>⊗</mo><mi>t</mi><mo>)</mo></mrow><mo>+</mo><msub><mrow><mi>G</mi></mrow><mrow><mi>n</mi><mi>t</mi></mrow></msub><mi>n</mi><mo>⊗</mo><mi>t</mi></mrow></math></span>, where <span><math><mi>γ</mi></math></span> is a material constant, <span><math><mi>t</mi></math></span> and <span><math><mi>n</mi></math></span> are appropriately defined orthonormal tangent vectors to the wall and <span><math><msub><mrow><mi>G</mi></mrow><mrow><mi>n</mi><mi>t</mi></mrow></msub></math></span> is a possibly non-zero component of <span><math><mi>G</mi></math></span> at the wall.</div></div>","PeriodicalId":14053,"journal":{"name":"International Journal of Engineering Science","volume":"209 ","pages":"Article 104162"},"PeriodicalIF":5.7000,"publicationDate":"2025-02-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Engineering Science","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0020722524001460","RegionNum":1,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
Fosdick and Fried (2021) proposed a generalized Navier–Stokes theory for studying the dynamics of incompressible fluids which, under certain flow conditions, may support incompatible distortion rates. Herein, we complete the development of a comprehensive boundary condition, at a fixed wall, for the incompatibility tensor of that theory; we clarify the physical conditions which express the presence of incompatibility at a wall and, thus, its transmission into the adjacent fluid. The final condition incorporates a constitutively prescribed threshold for the magnitude of the shear stress vector at the wall. For , . For , , where is a material constant, and are appropriately defined orthonormal tangent vectors to the wall and is a possibly non-zero component of at the wall.
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