FMDenaro |
September 20, 2012 10:52 |
Quote:
Originally Posted by Nick R
(Post 382781)
How do you define inertial force? You.previously said that it is the convective term in the navier stokes equations..that term is zero for.the.described channel flow.
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Your observation about the null lagrangian acceleration u * grad u is correct provided that you have a fully developed steady flow, this is only an academic framework. In the case you are citing it is the equilibrium of the isotropic to deviatoric part of the stress tensor that balance each other, since the isotropic part (the pressure) is of order rho*u^2 that leads to some misleading in the Re.
Again, I don't see the problem in the definition of Re as ratio between convective and diffusive fluxes (or convective to diffusive time) ... both do not vanish...
But the real flow in channel is far to be the Poiseulle solution, it is turbulent, with unsteady behaviour and inertial term always present, therefore I am used to define the Re in channel as rho*u_tau*H/mu wherein u_tau is the stress velocity that is defined by means of the pressure gradient
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