onsider a laminar boundary layer developed on a porous flat plate as shown in Figure 3, in which a uid is permeated through the plate with a superficial velocity vw. The von Karman momentum egral expression for the boundary layer on a porous plate is given as: -v.v. +fv.(v. -v, kty d rô dx and the ming the velocity profile in the boundary layer is of the form = a+b ary layer thickness of a Newtonian fluid flow will eventually reaches a constant thickness. an expression for this limiting thickness. Va y に Vnr Figure 3

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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Consider a laminar boundary layer developed on a porous flat plate as shown in Figure 3, in which a
liquid is permeated through the plate with a superficial velocity . The von Karman momentum
integral expression for the boundary layer on a porous plate is given as:
d ro
Te=v_vw + = [² v₂ (v_ - v₁ )dy
Р
dx
1 + b ( ² ) + c( ² ) ² ,
Vo
, and the
ssuming the velocity profile in the boundary layer is of the form
undary layer thickness of a Newtonian fluid flow will eventually reaches a constant thickness.
ive an expression for this limiting thickness.
Via
▬▬▬▬▬
Ynt
Figure 3
Transcribed Image Text:Consider a laminar boundary layer developed on a porous flat plate as shown in Figure 3, in which a liquid is permeated through the plate with a superficial velocity . The von Karman momentum integral expression for the boundary layer on a porous plate is given as: d ro Te=v_vw + = [² v₂ (v_ - v₁ )dy Р dx 1 + b ( ² ) + c( ² ) ² , Vo , and the ssuming the velocity profile in the boundary layer is of the form undary layer thickness of a Newtonian fluid flow will eventually reaches a constant thickness. ive an expression for this limiting thickness. Via ▬▬▬▬▬ Ynt Figure 3
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