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Physics I Chap 16. Fluid Dynamics Prof. WAN, Xin [email protected] http://zimp.zju.edu.cn/~xinwan/ Definitions Aerodynamics (gases in motion) Hydrodynamics (liquids in motion) – Blaise Pascal – Daniel Bernoulli, Hydrodynamica (1738) – Leonhard Euler – Lagrange, d’Alembert, Laplace, von Helmholtz Airplane, petroleum, weather, traffic 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 2 The Naïve Approach N particles ri(t), vi(t); interaction V(ri-rj) 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 3 Euler’s Solution For fluid at a point at a time: x, y, z, t , Field v x, y, z, t State of the fluid: described by parameters p, T. Laws of mechanics applied to particles, not to points in space. 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 4 Ideal Fluids Steady: velocity, density and pressure not change in time; no turbulence Incompressible: constant density Nonviscous: no internal friction between adjacent layers Irrotational: no particle rotation about center of mass 2017/5/22 Ferris Wheel at the Concorde Square, Paris http://zimp.zju.edu.cn/~xinwan/ 5 Streamlines Paths of particles P Q vP R vQ vR PQR v tangent to the streamline No crossing of streamlines 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 6 Mass Flux Tube of flow: bundle of streamlines Q P v1 A1 v2 A2 m1 m1 1 A1v1 t mass flux 1 A1v1 t1 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 7 Conservation of Mass IF: no sources and no sinks/drains 1 A1v1 2 A2 v2 constant A1v1 A2v2 constant, for incompressible fluid – Narrower tube == larger speed, fast – Wider tube == smaller speed, slow Example of equation of continuity. Also conservation of charge in E&M 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 8 Who Accelerates the Fluid? Acceleration due to pressure difference. Bernoulli’s Principle = Conservation of energy 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 9 Conservation of Energy Steady, incompressible, nonviscous, irrotational 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 10 Bernoulli’s Equation kinetic E, potential E, external work m A1 x1 A2 x2 1 1 2 p1 A1 x1 p2 A2 x2 mv2 mgy2 mv12 mgy1 2 2 1 2 1 2 p1 v1 gy1 p2 v2 gy2 2 2 1 2 p v gy constant 2 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 11 BEq in Everyday Life Open a faucet, the stream of water gets narrower as it falls. V1 V2 A1 A2 Velocity increases due to gravity as water flow down, thus, the area must get narrower. 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 12 Q & A on Bernoulli’s Eq. A bucket full of water. One hole and one pipe, both open at bottom. Out of which water flows faster? Same. It only depends on depth. 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 13 Bend it like Beckham Dynamic lift 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 14 Beckham, Applied Physicist Distance 25 m Initial v = 25 m/s Flight time 1s Spin at 10 rev/s Lift force ~ 4 N Ball mass ~ 400 g a = 10 m/s2 A swing of 5 m! ~ 5m Goal!! 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 15 Measuring Pressure… E. Torricelli: Mercury Barometer Patm gh p=0 patm 2017/5/22 h Patm h g http://zimp.zju.edu.cn/~xinwan/ 16 U-Tube Manometer pA 1 gh1 patm 2 gh2 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 17 The Venturi Meter Speed changes as diameter changes. Can be used to measure the speed of the fluid flow. 1 2 1 2 p1 v1 p2 v2 , 2 2 2017/5/22 v1 A1 v2 A2 http://zimp.zju.edu.cn/~xinwan/ 18 The Pitot Tube 1 2 pa va pb 2 pb pa gh 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 19 Viscous Fluid Flow Laminar flow: Following streamlines Fluids at low speeds Turbulent flow: Random or irreproducible Fluids at high speeds 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 20 Laminar Flow Fluid flows layer by layer with varying v. A y F, v A F = h A dv/dy 2017/5/22 h: coefficient of viscosity http://zimp.zju.edu.cn/~xinwan/ 21 Cylindrical Pipes r V(r) 2R P 2 2 v r (R r ) 4h L 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 22 Dimensional Analysis Goal: vc ∝ habDc D Dimensions: vc: LT-1 h: ML-1T-1 : ML-3 D: L 2017/5/22 v (F = h A dv/dy) http://zimp.zju.edu.cn/~xinwan/ 23 Reynolds Number a = 1, b = -1, c = -1 vc ~ h / (D) vc = R h / (D) Cylindrical pipes: Rc ~ 2000 Dv R h – For water, vc = 10 cm/s 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 24 A Remarkable Family Jakob Bernoulli (1654-1705) Johann Bernoulli (1667-1748), brother of Jokob Daniel Bernoulli (1700-1782), son of Johann; discovered Bernoulli’s Principle 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 25 Leonhard Euler (1707-83) Born in Basel on April 15, 1707 Studied under Johann Bernoulli Master’s degree (1724) – Comparing natural philosophy of Descartes and of Newton Petersburg Academy of Sciences (1727) Berlin Academy of Sciences (1741) Petersburg Academy of Sciences (1766) 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 26 Achievements of Euler Mathematics: calculus, differential equations, analytic and differential geometry, number theory, calculus of variations, … Physics: hydrodynamics; theories of heat, light, and sound, … Others: analytical mechanics, astronomy, optical instruments, … 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 27 Homework Fluid Statics: Page 348-349 Problems: 4, 14 2017/5/22 Fluid Dynamics: Page 369 Problems: 4, 14 http://zimp.zju.edu.cn/~xinwan/ 28 Zoom into a Fluid 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 29 Almond Blossom Almond Blossom by Vincent van Gogh, Rijksmuseum, Amsterdam 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 30 Brainteaser Q: What is greater than God, the dead eat it, and the living would die if they ate it!? Hint: For the theologically minded, please give a very short answer. 2017/5/22 http://zimp.zju.edu.cn/~xinwan/ 31