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In
fluid dynamics,
drag crisis is a phenomenon in which
drag coefficient drops off suddenly as
Reynolds number increases. This has been well studied for round bodies like
spheres and
cylinders. The drag coefficient of a sphere will change rapidly from about 0.5 to 0.2 at a Reynolds number in the range of 300000. This corresponds to the point where the flow pattern changes, leaving a narrower
turbulent wake. The behaviour is highly dependent on small differences in the condition of the surface of the sphere.