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Core Ag Engineering Principles – Session 1. Bernoulli’s Equation Pump Applications. Bernoulli’s Equation. Hydrodynamics (the fluid is moving) Incompressible fluid (liquids and gases at low pressures) Therefore changes in fluid density are not considered. Conservation of Mass.
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Core Ag Engineering Principles – Session 1 Bernoulli’s Equation Pump Applications
Bernoulli’s Equation • Hydrodynamics (the fluid is moving) • Incompressible fluid (liquids and gases at low pressures) • Therefore changes in fluid density are not considered
Conservation of Mass • If the rate of flow is constant at any point and there is no accumulation or depletion of fluid within the system, the principle of conservation of mass (where mass flow rate is in kg/s) requires:
Q is volumetric flow rate in m3/s A is cross-sectional area of pipe (m2) and V is the velocity of the fluid in m/s For incompressible fluids – density remains constant and the equation becomes:
Example • Water is flowing in a 15 cm ID pipe at a velocity of 0.3 m/s. The pipe enlarges to an inside diameter of 30 cm. What is the velocity in the larger section, the volumetric flow rate, and the mass flow rate?
Example D1 = 0.15 m D2 = 0.3 m V1 = 0.3 m/s V2 = ? How do we find V2?
Example • D1 = 15 cm ID D2 = 30 cm ID • V1 = 0.3 m/s V2 = ? • We know A1V1 = A2V2
Answer V2 = 0.075 m/s
Bernoulli’s Theorem • Since energy is neither created nor destroyed within the fluid system, the total energy of the fluid at one point in the system must equal the total energy at any other point plus any transfers of energy into or out of the system.
Bernoulli’s Theorem h = elevation of point 1 (m or ft) P1 = pressure (Pa or psi) = specific weight of fluid v = velocity of fluid
Bernoulli’s Theorem Special Cases • When system is open to the atmosphere, then P=0 if reference pressure is atmospheric (can be one P or both P’s)
When one V refers to a storage tank and the other V refers to a pipe, then V of tank <<<< V pipe and assumed zero • If no pump or fan is between the two points chosen, W=0
Example • Find the total energy (ft) at B; assume flow is frictionless A B 125’ C 75’ 25’
Example • Why is total energy in units of ft? • What are the typical units of energy? • How do we start the problem?
Example Total EnergyA = Total EnergyB Total EnergyB hA = 125’ = Total EnergyB
Example Find the velocity at point C. 0
Try it yourself: Water is pumped at the rate of 3 cfs through piping system shown. If the pump has a discharge pressure of 150 psig, to what elevation can the tank be raised? Assume the head loss due to friction is 10 feet. 9’ 1’ x’ pump 1’
Step 1 • Determine Reynolds number • Dynamic viscosity units • Diameter of pipe • Velocity • Density of fluid
Reynolds numbers: • < 2130 Laminar • > 4000 Turbulent • Affects what?
Reynolds numbers: • < 2130 Laminar • > 4000 Turbulent • Affects what? • The f in Darcy’s equation for friction loss in pipe • Laminar: f = 64 / Re • Turbulent: Colebrook equation or Moody diagram
Total F F = Fpipe + Fexpansion + Fcontraction+ Ffittings
Relative roughness is a function of the pipe material; for turbulent flow it is a value needed to use the Moody diagram (ε/D) along with the Reynolds number
Example • Find f if the relative roughness is 0.046 mm, pipe diameter is 5 cm, and the Reynolds number is 17312
Example • Find f if the relative roughness is 0.046 mm, pipe diameter is 5 cm, and the Reynolds number is 17312
Solution • ε / D = 0.000046 m / 0.05 m = 0.00092 • Re = 1.7 x 104 Re > 4000; turbulent flow – use Moody diagram
Find ε/D , move to left until hit dark black line – slide up line until intersect with Re #
Answer • f = 0.0285
Example • Milk at 20.2C is to be lifted 3.6 m through 10 m of sanitary pipe (2 cm ID pipe) that contains two Type A elbows. Milk in the lower reservoir enters the pipe through a type A entrance at the rate of 0.3 m3/min. Calculate F.
Calculate v = ? • Calculate v2 / 2g, because we’ll need this a lot
Viscosity = 2.13 x 10-3 Pa · s ρ = 1030 kg/m3
f = ? • Fpipe =
Ffittings= • Fexpansion = • Fcontraction=