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Jean Le Rond D'Alembert: A New Theory of the Resistance of FluidsGeneral Principles of the Pressure Fluids, in Motion or at Rest

Jean Le Rond D'Alembert: A New Theory of the Resistance of Fluids: General Principles of the... [21. Let MNGH (Fig. 3.1) be a homogeneous fluid without weight, and that either it is of an indefinite extension or enclosed in a reservoir of any size and shape. Place a solid body BCDE anywhere one wishes inside this fluid, taking around that body a fluid portion limited by the surface FOKL and assuming that all the particles of either the fluid or the solid contained by the FOKL surface are impelled by such forces that an equilibrium exists between the fluid and the solid. The pressure that the fluid exerts on any point D of the solid body is impelled.] http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.png

Jean Le Rond D'Alembert: A New Theory of the Resistance of FluidsGeneral Principles of the Pressure Fluids, in Motion or at Rest

Part of the Studies in History and Philosophy of Science Book Series (volume 47)
Editors: Calero, Julián Simón

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Publisher
Springer International Publishing
Copyright
© Springer International Publishing AG 2018
ISBN
978-3-319-67999-0
Pages
29 –37
DOI
10.1007/978-3-319-68000-2_3
Publisher site
See Chapter on Publisher Site

Abstract

[21. Let MNGH (Fig. 3.1) be a homogeneous fluid without weight, and that either it is of an indefinite extension or enclosed in a reservoir of any size and shape. Place a solid body BCDE anywhere one wishes inside this fluid, taking around that body a fluid portion limited by the surface FOKL and assuming that all the particles of either the fluid or the solid contained by the FOKL surface are impelled by such forces that an equilibrium exists between the fluid and the solid. The pressure that the fluid exerts on any point D of the solid body is impelled.]

Published: Jan 13, 2018

Keywords: Homogeneous Fluid; αF Βγ; Indefinite Length; Equal Velocity; Slices

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