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, 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

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