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Physics · Ch 2 — Mechanical Properties of Fluids

Critical Velocity and Reynolds Number

2.6

Critical Velocity and Reynolds Number

The flow of a fluid, whether streamline or turbulent, is distinguished on the basis of the velocity of the flow. The velocity beyond which a streamline flow becomes turbulent is called the critical velocity. According to Osborne Reynolds (1842-1912), the critical velocity is given by:

vc=Rn ηρ d— (2.32)v_c = \dfrac{R_n\,\eta}{\rho\,d} \qquad \text{--- (2.32)}

where vcv_c is the critical velocity of the fluid, RnR_n is the Reynolds number, η is the fluid's coefficient of viscosity, ρ is the fluid's density, and d is the diameter of the tube through which it is flowing. Equation (2.32) can be rearranged to give the Reynolds number itself:

Rn=ρ vc dη— (2.33)R_n = \dfrac{\rho\,v_c\,d}{\eta} \qquad \text{--- (2.33)} …