Consider the steady, isothermal, irrotational flow of an incompressible frictionless fluid subject only to a body force characterized by a potential D, where F,=- V (in units of force/volume). Since the fluid is frictionless, the only surface force is due to pressure, F, : =-pn . Вy completing a momentum balance on a material volume of fluid subject to the constraints listed above, derive Bernouilli's law, P + ½pv² + D = constant along a fluid streamline.
Consider the steady, isothermal, irrotational flow of an incompressible frictionless fluid subject only to a body force characterized by a potential D, where F,=- V (in units of force/volume). Since the fluid is frictionless, the only surface force is due to pressure, F, : =-pn . Вy completing a momentum balance on a material volume of fluid subject to the constraints listed above, derive Bernouilli's law, P + ½pv² + D = constant along a fluid streamline.
Introduction to Chemical Engineering Thermodynamics
8th Edition
ISBN:9781259696527
Author:J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
Publisher:J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
Chapter1: Introduction
Section: Chapter Questions
Problem 1.1P
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Transcribed Image Text:Consider the steady, isothermal, irrotational flow of an incompressible frictionless fluid subject
only to a body force characterized by a potential O, where F,=- V@ (in units of force/volume).
Since the fluid is frictionless, the only surface force is due to pressure, F =-pn. By
completing a momentum balance on a material volume of fluid subject to the constraints listed
above, derive Bernouilli's law,
P + ½pv² + O = constant
along a fluid streamline.
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