PHYS 1441 – Section 004 Lecture #21 Monday, Apr. 19, 2004 Dr. Jaehoon Yu • • • • Buoyant Force and Archimedes’ Principle Flow Rate and Equation of Continuity Bernoulli’s Equation Simple Harmonic Motion Quiz next Wednesday, Apr. 28! Monday, Apr. 19, 2004 PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 1 Announcements • Quiz stats – Average : 48.4/90 53.8/100 – Top score: 80/90 – Previous quiz scores: 38.2, 41, 57.9 • Next quiz on Wednesday, Apr. 28 – Covers: ch. 10.4 – ch.11, including all that are covered in the lecture • Mid-term grade one-on-one discussion – 11 have not done this yet – One more opportunity today Monday, Apr. 19, 2004 PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 2 Buoyant Forces and Archimedes’ Principle Why is it so hard to put a beach ball under water while a piece of small steel sinks in the water? The water exerts force on an object immersed in the water. This force is called Buoyant force. How does the The magnitude of the buoyant force always equals the weight of Buoyant force work? the fluid in the volume displaced by the submerged object. This is called, Archimedes’ principle. What does this mean? Let‘s consider a cube whose height is h and is filled with fluid and at its equilibrium. Then the weight Mg is balanced by the buoyant force B. B Fg Mg And the pressure at the bottom of the cube is larger than the top by rgh. h Mg B Monday, Apr. 19, 2004 Therefore, P B / A rgh Where Mg is the B PA rghA rVg weight of the fluid. B Fg rVg Mg PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 3 More Archimedes’ Principle Let’s consider buoyant forces in two special cases. Case 1: Totally submerged object Let’s consider an object of mass M, with density r0, is immersed in the fluid with density rf . The magnitude of the buoyant force is B r f Vg The weight of the object is Fg Mg r 0Vg h Mg B Therefore total force of the system is F B Fg r f r 0 Vg What does this tell you? Monday, Apr. 19, 2004 The total force applies to different directions depending on the difference of the density between the object and the fluid. 1. If the density of the object is smaller than the density of the fluid, the buoyant force will push the object up to the surface. 2. If the density of the object is larger that the fluid’s, the object will sink to the bottom of the fluid. PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 4 More Archimedes’ Principle Case 2: Floating object h Mg B Let’s consider an object of mass M, with density r0, is in static equilibrium floating on the surface of the fluid with density rf , and the volume submerged in the fluid is Vf. The magnitude of the buoyant force is The weight of the object is Therefore total force of the system is Since the system is in static equilibrium B r fVf g Fg Mg r 0V0 g F B Fg r f V f g r 0V0 g 0 r f V f g r0V0 g r0 V f rf V0 What does this tell you? Monday, Apr. 19, 2004 Since the object is floating its density is always smaller than that of the fluid. The ratio of the densities between the fluid and the object determines the submerged volume under the surface. PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 5 Example for Archimedes’ Principle Archimedes was asked to determine the purity of the gold used in the crown. The legend says that he solved this problem by weighing the crown in air and in water. Suppose the scale read 7.84N in air and 6.86N in water. What should he have to tell the king about the purity of the gold in the crown? In the air the tension exerted by the scale on the object is the weight of the crown Tair mg 7.84 N Twater mg B 6.86 N In the water the tension exerted by the scale on the object is B Tair Twater 0.98N Therefore the buoyant force B is Since the buoyant force B is B r wVw g r wVc g 0.98N The volume of the displaced 0.98 N 0.98 4 3 V V 1 . 0 10 m c w water by the crown is r w g 1000 9.8 Therefore the density of mc mc g 7.84 7.84 3 3 8 . 3 10 kg / m r 4 the crown is c V Vc g Vc g 1.0 10 9.8 c 3kg/m 3, this Spring Monday,the Apr.density 19, 2004of pure gold is 19.3x10 PHYS 1441-004, 6 Since crown2004 is either not made of pure gold or hollow. Dr. Jaehoon Yu Example for Buoyant Force What fraction of an iceberg is submerged in the sea water? Let’s assume that the total volume of the iceberg is Vi. Then the weight of the iceberg Fgi is Fgi riVi g Let’s then assume that the volume of the iceberg submerged in the sea water is Vw. The buoyant force B caused by the displaced water becomes B r wVw g Since the whole system is at its static equilibrium, we obtain Therefore the fraction of the volume of the iceberg submerged under the surface of the sea water is riVi g r wVw g Vw r i 917kg / m3 0.890 3 Vi r w 1030kg / m About 90% of the entire iceberg is submerged in the water!!! Monday, Apr. 19, 2004 PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 7 Flow Rate and the Equation of Continuity Study of fluid in motion: Fluid Dynamics If the fluid is water: Water dynamics?? Hydro-dynamics •Streamline or Laminar flow: Each particle of the fluid Two main types of flow follows a smooth path, a streamline •Turbulent flow: Erratic, small, whirlpool-like circles called eddy current or eddies which absorbs a lot of energy Flow rate: the mass of fluid that passes a given point per unit time m / t m1 r1V1 r1 A1l1 r1 A1v1 t t t since the total flow must be conserved m1 m2 r1 A1v1 r 2 A2 v2 t t Equation of Continuity Monday, Apr. 19, 2004 PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 8 Example for Equation of Continuity How large must a heating duct be if air moving at 3.0m/s along it can replenish the air every 15 minutes, in a room of 300m3 volume? Assume the air’s density remains constant. Using equation of continuity r1 A1v1 r 2 A2 v2 Since the air density is constant A1v1 A2 v2 Now let’s imagine the room as the large section of the duct A2l2 / t V2 A2 v2 300 A1 0.11m 2 v1 v1 t v1 3.0 900 Monday, Apr. 19, 2004 PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 9 Bernoulli’s Equation Bernoulli’s Principle: Where the velocity of fluid is high, the pressure is low, and where the velocity is low, the pressure is high. Amount of work done by the force, F1, that exerts pressure, P1, at point 1 W1 F1l1 P1 A1l1 Amount of work done on the other section of the fluid is W2 P2 A2 l2 Work done by the gravitational force to move the fluid mass, m, from y1 to y2 is W3 mg y2 y1 Monday, Apr. 19, 2004 PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 10 Bernoulli’s Equation cont’d The net work done on the fluid is W W1 W2 W3 P1 A1l1 P2 A2 l2 mgy2 mgy1 From the work-energy principle 1 1 2 mv2 mv12 P1 A1l1 P2 A2 l2 mgy2 mgy1 2 2 Since mass, m, is contained in the volume that flowed in the motion A1l1 A2 l2 Thus, and m r A1l1 r A2 l2 1 1 2 2 r A2 l2 v2 r A1l1v1 2 2 P1 A1l1 P2 A2 l2 r A2 l2 gy2 r A1l1 gy1 Monday, Apr. 19, 2004 PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 11 Bernoulli’s Equation cont’d Since 1 1 r A2 l2 v22 r A1l1v12 P1 A1l1 P2 A2 l2 r A2 l2 gy2 r A1l1 gy1 2 2 We obtain Reorganize P1 1 2 1 2 r v2 r v1 P1 P2 r gy2 r gy1 2 2 1 2 1 2 Bernoulli’s r v1 r gy1 P2 r v2 r gy2 Equation 2 2 Thus, for any two points in the flow 1 2 P1 r v1 r gy1 const. 2 For static fluid P2 P1 r g y1 y2 P1 r gh 1 2 2 P P r v v 2 1 1 2 For the same heights 2 Pascal’s Law The pressure at the faster section of the fluid is smaller than slower section. Monday, Apr. 19, 2004 PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 12 Example for Bernoulli’s Equation Water circulates throughout a house in a hot-water heating system. If the water is pumped at a speed of 0.5m/s through a 4.0cm diameter pipe in the basement under a pressure of 3.0atm, what will be the flow speed and pressure in a 2.6cm diameter pipe on the second 5.0m above? Assume the pipes do not divide into branches. Using the equation of continuity, flow speed on the second floor is 2 A1v1 r12 v1 0.020 v2 0.5 1.2m / s 2 A2 r2 0.013 Using Bernoulli’s equation, the pressure in the pipe on the second floor is 1 P2 P1 r v12 v22 r g y1 y2 2 1 5 3.0 10 1103 0.52 1.22 1103 9.8 5 2 2.5 105 N / m 2 Monday, Apr. 19, 2004 PHYS 1441-004, Spring 2004 Dr. Jaehoon Yu 13