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Published byLeon Casey Modified over 9 years ago
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CIEG 305 DERIVATION OF BERNOULLI”S EQN FROM LINEAR MOMENTUM ALONG A STREAMLINE P+dP A A+dA V,ρ P ds dz θ V+dV ρ+dρ dW≈ρgdVol Gory Details 1 2
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Take a narrow stream tube at some angle (shown on previous slide Require cross-sections to be small to that we take P and V essentially constant Neglect friction and assume incompressible. Now conserve mass using RTT for control volume defined by stream tube
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OR REFERENCING EVERYTHING TO STATION 1
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FROM MASS CONSERVATION AND ASSUMPTION THAT VALUES ARE MORE OR LESS EQUAL Product rule This is the differential form of mass conservation along streamline
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LINEAR MOMENTUM EQUATION IN STREAMWISE DIRECTION The last part comes from ugly chain rule, product rule and substitution of mass conservation
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WHAT ARE THE FORCES?? GRAVITY PRESSURE
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SUBSTITUTE INTO THE LINEAR MOMENTUM EQUATION By mass continuity
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Divide by ρA and rearrange THIS IS BERNOULLI’S EQUATION FOR UNSTEADY FRICTIONLESS FLOW ALONG A STREAMLINE INTEGRATE ALONG STREAMLINE
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If we consider only steady state and incompressible flow THIS IS BERNOULLI’S EQUATION FOR STEADY, FRICTIONLESS, INCOMPRESSIBLE FLOW ALONG A STREAMLINE
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