✦ LIBER ✦

Variational principle for three-dimensional steady-state flows of an ideal fluid

✍ Scribed by V.I Arnol'd

Publisher: Elsevier Science
Year: 1965
Tongue: English
Weight: 441 KB
Volume: 29
Category: Article
ISSN: 0021-8928
DOI: 10.1016/0021-8928(65)90119-x

No coin nor oath required. For personal study only.

📜 SIMILAR VOLUMES

On the topology of three-dimensional ste

On the topology of three-dimensional steady flows of an ideal fluid

✍ V.I. Arnol'd 📂 Article 📅 1966 🏛 Elsevier Science 🌐 English ⚖ 226 KB

Performance analysis of IDEAL algorithm

Performance analysis of IDEAL algorithm for three-dimensional incompressible fluid flow and heat transfer problems

✍ Dong-Liang Sun; Zhi-Guo Qu; Ya-Ling He; Wen-Quan Tao 📂 Article 📅 2009 🏛 John Wiley and Sons 🌐 English ⚖ 288 KB

A second-order finite-difference scheme

A second-order finite-difference scheme for computing three-dimensional supersonic flows of an ideal gas

✍ M.K. Aukin; R.K. Tagirov 📂 Article 📅 1989 🏛 Elsevier Science ⚖ 627 KB

Note on the stability of three-dimension

Note on the stability of three-dimensional flows of an ideal fluid: PMM vol. 37, n≗3, 1973, pp. 557–558

✍ N.N. Bogdat'eva; L.A. Dikii 📂 Article 📅 1973 🏛 Elsevier Science 🌐 English ⚖ 162 KB

An extremum variational principle and er

An extremum variational principle and error estimate procedure for radial flow of a viscous fluid between porous discs

✍ DJ.S. Djukic; T.M. Atanackovic 📂 Article 📅 1987 🏛 Elsevier Science 🌐 English ⚖ 381 KB

On the steady state fractionation of mul

On the steady state fractionation of multicomponent and complex mixtures in an ideal cascade: Part VI—The effect of variations of the relative volatilities, the flow rates and the plate efficiencies

✍ Andreas Acrivos; Neal R. Amundson 📂 Article 📅 1955 🏛 Elsevier Science 🌐 English ⚖ 467 KB

An approximate yet standard procedure, the perturbation method, is used to solve analytically the equation for the steafiy state fractionation of multicomponent and complex mixtures in non-ideal cascades. It is shown that the formulae are easily adaptable to numerical evaluation. The perturbation m