1 / 33

Fluid Dynamics

Fluid Dynamics. Two Parts Fluid Flow Bernoulli’s Equation and Applications. Assumptions for Fluid Flow:. Non-viscous. (isn’t “sticky”) I ncompressible (constant ρ ) All particles in cross section travel at the same speed (flow rate) Flow is laminar (no turbulence). Streamline flow.

anoki
Download Presentation

Fluid Dynamics

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Fluid Dynamics Two Parts • Fluid Flow • Bernoulli’s Equation and Applications

  2. Assumptions for Fluid Flow: Non-viscous. (isn’t “sticky”) Incompressible (constant ρ) All particles in cross section travel at the same speed (flow rate) Flow is laminar (no turbulence) Streamline flow Turbulent flow

  3. Laminar Flow Laminar flow, type of fluid (gas or liquid) flow in which the fluid travels smoothly or in regular paths Laminar flow over a horizontal surface may be thought of as consisting of thin layers, or laminae, all parallel to each other.

  4. Laminar Flow • Video:

  5. Flow Rate Flow Rate (ƒ): Volume of fluid that passes a particular point in a given time Units used to measure Flow Rate = m³/sec Equation for: Flow Rate ƒ = Aν = (m2)(m/s) (A = cross sectional area) (ν= velocity of fluid)

  6. vt A Volume = A(vt) Rate of flow = velocity x area Rate of Flow

  7. Since A1 > A2… For an incompressible, frictionless fluid, the velocity increases when the cross-section decreases:

  8. Continuity Equation Flow rates are the same at all points along a closed pipe Continuity Equation: ƒ₁ = ƒ₂ A₁ν₁ = A₂ν₂ Reminder: the equation for Area of a circle: A = πr²

  9. PHet • Fluid Flow

  10. Question: Water travels through a 9.6 cm diameter fire hose with a speed of 1.3 m/s. At the end of the hose, the water flows out through a nozzle whose diameter is 2.5 cm. What is the speed of the water coming out of the nozzle?

  11. Venturi Meter The higher the velocity in the constriction at Region-2, the lower the pressure... Wait what?

  12. Venturi Effect

  13. Venturi Effect

  14. Airplane Wings

  15. Airplane Wings

  16. How do Plane’s Fly Video

  17. The Physics of Sailing Video http://science.kqed.org/quest/video/the-physics-of-sailing/

  18. Question A small ranger vehicle has a soft, ragtop roof. When the car is at rest the roof is flat. When the car is cruising at highway speeds with its windows rolled up, does the roof • bow upward • remain flat • bow downward?

  19. Question A small ranger vehicle has a soft, ragtop roof. When the car is at rest the roof is flat. When the car is cruising at highway speeds with its windows rolled up, does the roof • bow upward • remain flat • bow downward?

  20. Fluid Flow Questions • MC - 4,14,21,42,47 • Homework: Watch Bernoulli Video • MOST IMPORTANTLY: Paper Airplane Competition next class Go to: http://www.funpaperairplanes.com/index.html • Pick a plane and build it for the start of class • Make TWO of the same design • Planes will be thrown in players hall • Winner will be determined by displacement from initial throw

  21. Sports Science • Record Paper Airplane

  22. Conservation of Energy of Fluids within a Pipe Bernoulli's Principle PRESSURE plus ENERGY is CONSTANT! • P + E = P + E • P + U + K = P + U + K • P + ρgh+ ½ρν² = P + ρgh + ½ρν² This hold at ANY point! P1 + ρgh1 + ½ρν1² = P2 + ρgh2+ ½ρν2²

  23. Bernuolli Effect • High Velocity: _____ Pressure • Low Velocity: _____ Pressure

  24. Bernuolli Effect • High Velocity: LOW Pressure • Low Velocity: HIGH Pressure

  25. Horizontal Pipe Special Case #1 – Horizontal Pipe Horizontal Pipe (h1 = h2)

  26. Question Suppose the pressure in the fire hose is 350 kPa. What is the pressure in the nozzle? ν1 = 1.3 m/s ν2 = 19.17 m/s

  27. Special Case #2 – Constant Velocity Constant velocity (ν1= ν2) Notice how a difficult problem becomes easier when we remove constants!

  28. Question Water flows with constant speed through a garden hose that goes up a step 20.0 cm high. If the water pressure is 143 kPa at the bottom of the step, what is its pressure at the top of the step? ν1 = ν2

  29. Special Case #3 – Fluids at Rest P1 - P2 = rgh2 - rgh1 DP = rg(h2 - h1) We have already seen this!

  30. h h2 h1 Torricelli’s theorem: Special Case #4 – No Change in Pressure Know as Torricelli’s Theorem v2 0

  31. h Question: A dam springs a leak at a point 20.0 m below the surface. What is the emergent velocity? v = 19.8m/s2

  32. Streamline Fluid Flow in Pipe: Fluid at Rest: Horizontal Pipe (h1 = h2) PA - PB = rgh Bernoulli’s Theorem: Torricelli’s theorem: Summary of Hydrodynamics

  33. Bernoulli’s Principal • MC: 5,13,22,25,27,28,33,36,37,44 • Homework: Review Free Response Questions Posted on Website • Next Class: Hydrodynamics Quiz

More Related