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Equation of continuity and Bernoulli’s Principle (Ch. 10)

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Presentation on theme: "Equation of continuity and Bernoulli’s Principle (Ch. 10)"— Presentation transcript:

1 Equation of continuity and Bernoulli’s Principle (Ch. 10)
Owen von Kugelgen Head-Royce School

2 Moving Fluids Continuity Principle A1v1 = A2v2
Bernoulli’s Principle P1 + Dgh1 + (1/2)Dv12 = P2 + Dgh2 + (1/2)Dv22 (really just conservation of energy!)

3 Continuity Principle A1v1 = A2v2
When the diameter of a pipe decreases, the speed of the water increases (imagine a garden hose)

4 Continuity Principle A1v1 = A2v2
∆x2 ∆x1 Vol1/t = Vol2/t A1 ∆x1 / t = A2 ∆x2 / t A1v1 = A2v2

5 Can we apply energy concepts to fluids?
PE = mgh PE/Vol = Dgh Pressure = F/A P = (F*d)/Vol = W/Vol P = Energy/Vol KE = (1/2)mv2 KE/Vol = (1/2)Dv2

6 Bernoulli’sPrinciple

7 Bernoulli’s Principle
h P1 P2 = P1 + Dgh ∆Pressure = ∆PE/V = Dg∆h

8 Bernoulli’s Principle
v2 P1 P2 v1 P1 + Dgh1+ (1/2)Dv12 = P2 + Dgh2 + (1/2)Dv22 P1 = P2 + (1/2)Dv22 - (1/2)Dv12 P1 = P2 + (1/2)D[v22 - v12] Due to the continuity principle: v2 > v1 so P1 > P2

9 Bernoulli’s Principle
Conceptual meaning: Higher fluid speed produces lower pressure This helps wings lift balls curve atomizers and carburetors Do their job

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12 Wing lift The air across the top of a conventional airfoil experiences constricted flow lines and increased air speed relative to the wing. This causes a decrease in pressure on the top according to the Bernoulli equation and provides a lift force

13 Curve Ball


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