Question: In this chapter, we discuss solid body rotation (Fig. P10108) as an example of an inviscid flow that is also rotational. The velocity components are

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, uθ = ωr, and uz = 0. Compute the viscous term of the θ-component of the Navier–Stokes equation, and discuss. Verify that this velocity field is indeed rotational by computing the z-component of vorticity.


FIGURE P10–108

Up 4 Ug = wr all

Up 4 Ug = wr all

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