Transcription of Fluid Flow & Bernoulli's Equation
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MET 330 Introduction to Fluid PowerOnline NotesFluid Flow & Bernoulli's EquationVelocity ProflesPreviously we said that the velocity of hydraulic Fluid in a pipe is theflow rate times the cross-sectional area of the pipe: v=QA. Actually,this velocity is the average velocity of all the Fluid molecules movingthrough the pipe. At low flow rates, all of the molecules move parallel tothe axis of the pipe, and we have laminar flow. Molecules at thecenterline move fastest, while Fluid molecules at the wall remainattached to the wall. The velocity profile is higher flow rates, Fluid molecules do not follow straight paths;instead, eddies form in the flowstream, and we have turbulent at the centerline move fastest, but the velocity profile issomewhat flattened. Notice that there is a velocity at the wall, so surfaceroughness affects the flow. In turbulent flow, the rougher the pipe wall,the greater the friction and pressure drop. Turbulence is undesirable in ahydraulic system because it increases the pressure drop in a pipe, so it isbest to design hydraulic systems with laminar to Bernoulli's EquationThe 18th century Swiss mathematician Daniel bernoulli developed an Equation for calculating pressures and velocities in a flowstream.
MET 330 Introduction to Fluid Power Online Notes NR<2000 we have laminar flow. The textbook provides four equations for Reynolds number: two in US Customary, two in SI, each set with either absolute
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