In this chapter, we discuss solid body rotation (Fig. P10108) as an example of an inviscid flow
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In this chapter, we discuss solid body rotation (Fig. P10–108) as an example of an inviscid flow that is also rotational. The velocity components are ur = 0, u_{θ} = ωr, and u_{z} = 0. Compute the viscous term of the θcomponent of the Navier–Stokes equation, and discuss. Verify that this velocity field is indeed rotational by computing the zcomponent of vorticity.
FIGURE P10–108
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The viscous term of the component of the NavierStokes equation is given by u r 1 r u r u z where is ...View the full answer
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Related Book For
Fluid Mechanics Fundamentals And Applications
ISBN: 9780073380322
3rd Edition
Authors: Yunus Cengel, John Cimbala
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