Imagine a steady, two-dimensional, incompressible flow that is purely circular in the xy- or r-plane. In other
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Imagine a steady, two-dimensional, incompressible flow that is purely circular in the xy- or rθ-plane. In other words, velocity component uθ is nonzero, but ur is zero everywhere (Fig. P9–33). What is the most general form of velocity component uθ that does not violate conservation of mass?
FIGURE P9–33
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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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