Viscous friction with Bernoulli We can include the effect of viscous friction in Bernoulli’s equation by adding a term for the thermal energy generated by the viscous retarding force exerted on the fluid. Show that the term to be added to Eq. (11.5) for flow in a vessel of uniform cross-sectional area A is
where v is the average speed of the fluid of viscosity h along the center of a pipe whose length is l.
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