From Navier to Stokes: Commemorating the Bicentenary of Navier’s Equation on the Lay of Fluid Motion

IF 1.8 Q3 MECHANICS
Fluids Pub Date : 2024-01-06 DOI:10.3390/fluids9010015
Aldo Tamburrino
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引用次数: 0

Abstract

The article presents a summarised history of the equations governing fluid motion, known as the Navier–Stokes equations. It starts with the work of Castelli, who established the continuity equation in 1628. The determination of fluid flow resistance was a topic that involved the brightest minds of the 17th and 18th centuries. Navier’s contribution consisted of the incorporation of molecular attraction effects into Euler’s equation, giving rise to an additional term associated with resistance. However, his analysis was not the only one. This continued until 1850, when Stokes firmly established the boundary conditions that must be applied to the differential equations of motion, specifically stating the non-slip condition of the fluid in contact with a solid surface. With this article, the author wants to commemorate the bicentennial of the publication of “Sur les Lois du Mouvement des Fluides” by Navier in the Mémoires de l’Académie Royale des Sciences de l’Institut de France.
从纳维叶到斯托克斯:纪念纳维叶流体运动方程诞生二百周年
文章概述了流体运动方程(即纳维-斯托克斯方程)的历史。文章从卡斯泰利的工作开始,他于 1628 年建立了连续性方程。确定流体流动阻力是 17 世纪和 18 世纪最聪明的人都在研究的课题。纳维叶的贡献在于将分子吸引效应纳入欧拉方程,从而产生了与阻力相关的附加项。然而,他的分析并不是唯一的分析。直到 1850 年,斯托克斯确定了必须应用于运动微分方程的边界条件,特别说明了流体与固体表面接触时的非滑动条件。通过这篇文章,作者希望纪念纳维耶在《法兰西学院皇家科学院备忘录》上发表《流体运动规律》两百周年。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Fluids
Fluids Engineering-Mechanical Engineering
CiteScore
3.40
自引率
10.50%
发文量
326
审稿时长
12 weeks
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