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Physics 1B03summer-Lecture 13 Final Exam April 18 2 hours long – 30 MC questions Covers all material with approximately equal weight, up to and including.

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Presentation on theme: "Physics 1B03summer-Lecture 13 Final Exam April 18 2 hours long – 30 MC questions Covers all material with approximately equal weight, up to and including."— Presentation transcript:

1 Physics 1B03summer-Lecture 13 Final Exam April 18 2 hours long – 30 MC questions Covers all material with approximately equal weight, up to and including today’s final lecture on fluids.

2 Physics 1B03summer-Lecture 13 Fluid Dynamics Equation of Continuity Bernoulli’s equation and examples

3 Physics 1B03summer-Lecture 13 Fluid Dynamics Approximations: 1)no viscosity (frictionless flow) 2)steady, “laminar” flow. If the flow is turbulent, mechanical energy is lost (converted to thermal energy). 3)“incompressible” fluid. Sufficiently accurate for gases if pressure differences are small.

4 Physics 1B03summer-Lecture 13 Streamlines -the paths followed by particles in steady flow -velocity is parallel to the streamline - particles never cross streamlines; the streamlines mark out imaginary “tubes of flow” area A 1 speed v 1 area A 2 speed v2

5 Physics 1B03summer-Lecture 13 Equation of Continuity “Volume flow rate” (volume per unit time) = (cross-sectional area)  (linear velocity) “Mass flow rate” (mass per unit time) = (density)  (volume flow rate) So, if mass in = mass out, then  1 A 1 v 1 =  2 A 2 v 2  Av = mass flow rate = constant or for steady flow. “Incompressible” fluids (density remains uniform): cancel out density to get Volume flow rate = constant or A 1 v 1 = A 2 v 2

6 Physics 1B03summer-Lecture 13 radius r 1 = 10mm radius r 2 = 5mm A fluid if flowing through a pipe of 10mm radius at a velocity of 10m/s. How fast will it be flowing if the pipe narrows to 5mm in radius ?

7 Physics 1B03summer-Lecture 13 Bernoulli’s Equation: work and energy in fluids Conditions: steady flow, incompressible fluid. Look at energy balance along a streamline: Change in (kinetic energy/volume) + change in (potential energy/volume) = (net work by pressure)/volume then, or, Note: the above equation looks similar what we have seen before if we replace ρ by m.

8 Physics 1B03summer-Lecture 13 Example a) What is the velocity of the water leaving the little hole b) How far (horizontally) from the hole does the water hit the ground? d h x

9 Physics 1B03summer-Lecture 13 Example What is the speed of the water leaving the hole in the tank? gauge pressure P 0 h v

10 Physics 1B03summer-Lecture 13 Example Water moving at 10m/s through a 1m radius pipe at a pressure of 50kPa. It then falls 50m and goes into a 0.3m radius pipe. What is the water pressure at the bottom ? h


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