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Announcements Exams will be returned at the end of class.

Announcements Exams will be returned at the end of class. You may rework the exam for up to 10 extra credit points. Turn in your old exam and your new work (clearly indicated). Due 11/11/03. You may sign up for presentations if there is sufficient interest.

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Announcements Exams will be returned at the end of class.

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  1. Announcements • Exams will be returned at the end of class. • You may rework the exam for up to 10 extra credit points. Turn in your old exam and your new work (clearly indicated). Due 11/11/03. • You may sign up for presentations if there is sufficient interest. • Today’s lecture – fluids – Chapter 15 • Static fluids – buoyant force • Fluid flow PHY 113 -- Lecture 16

  2. The physics of fluids. • Fluids include liquids (usually “incompressible) and gases (highly “compressible”). • Fluids obey Newton’s equations of motion, but because they move within their containers, the application of Newton’s laws to fluids introduces some new forms. • Pressure: P=force/area 1 (N/m2) = 1 Pascal • Density: r =mass/volume 1 kg/m3 = 0.001 gm/ml Note: In this chapter Ppressure (NOT MOMENTUM) PHY 113 -- Lecture 16

  3. Pressure exerted by air at sea-level 1 atm = 1.013x105 Pa Example: What is the force exerted by 1 atm of air pressure on a circular area of radius 0.08m? F = PA = 1.013x105 Pa x p(0.08m)2 = 2040 N Pressure exerted by a fluid acts in all directions. PHY 113 -- Lecture 16

  4. Density: r =mass/volume Effects of the weight of a fluid: P(y+Dy) rgDy y P(y) Note: In this formulation +y is defined to be in the up direction. PHY 113 -- Lecture 16

  5. For an “incompressible” fluid (such as mercury): r = 13.585 x 103 kg/m3 (constant) Example: r = 13.595 x 103 kg/m3 PHY 113 -- Lecture 16

  6. Weather report: PHY 113 -- Lecture 16

  7. Question: Consider the same setup, but replace fluid with water (r = 1000 kg/m3). What is h? r = 1000kg/m3 PHY 113 -- Lecture 16

  8. Buoyant force for fluid acting on a solid: FB=rfluidVdisplacedg FB - mg = 0 rfluidVsubmergedg -rsolidVsolidg = 0 A Dy mg PHY 113 -- Lecture 16

  9. Suppose you have a boat which floats in a fresh water lake, with 50% of it submerged below the water. If you float in the same boat in salt water, which of the following would be true? • More than 50% of the boat will be below the salt water. • Less than 50% of the boat will be below the salt water. • The submersion fraction depends upon the boat's total mass and volume. • The submersion fraction depends upon the barometric pressure. PHY 113 -- Lecture 16

  10. Archimede’s method of finding the density of the King’s “gold” crown Wwater Wair PHY 113 -- Lecture 16

  11. Effects of the weight of a “compressible” fluid on pressure. y-y0(mi) P (atm) PHY 113 -- Lecture 16

  12. Summary: Application of Newton’s second law to fluid (near Earth’s surface) PHY 113 -- Lecture 16

  13. Peer instruction question Suppose that a caterer packed some food in an air tight container with a flexible top at sea-level. This food was loaded on to an airplane with a cruising altitude of ~6 mi above the earth’s surface. Assuming that the airplane cabin is imperfectly pressurized, what do you expect the container to look like during the flight? (A) (B) (C) PHY 113 -- Lecture 16

  14. Peer instruction question Suppose that a caterer packed some food in an air tight container with a flexible top at sea-level. This food was loaded on to a submarine which typically submerges at 200m below sea level. Assuming that the submarine cabin is imperfectly pressurized, what do you expect the container to look like during the submersion? (A) (B) (C) PHY 113 -- Lecture 16

  15. Physics of flowing (incompressible)* fluids A1v1Dt=A2v2Dt *Later will generalize to compressible fluids in “streamline” flow. PHY 113 -- Lecture 16

  16. Energetics of fluids: Dx1 =v1Dt Dx2 =v2Dt A1 Dx1= A2 Dx2 m = r A1 Dx1 K2 + U2 = K1 + U1 +W12 ½ mv22 + mgh2 = ½ mv12 + mgh1 + (P1 A1 Dx1– P2 A2 Dx2) P2 + ½ rv22 + rgh2 = P1 + ½ rv12 + rgh1 PHY 113 -- Lecture 16

  17. Bernoulli’s equation: P2 + ½ rv22 + rgh2 = P1 + ½ rv12 + rgh1 Example: Suppose we know A1, A2, r, P, y1, y2 P + ½ rv22 + rgy2 = P0 + ½ rv12 + rgy1 PHY 113 -- Lecture 16

  18. Streamline flow of air around an airplane wing: P2 + ½ rv22 + rgh2 = P1 + ½ rv12 + rgh1 Flift=(P2-P1)A P1 v1 Example: v1 = 270 m/s v2 = 260 m/s r = 0.6 kg/m3 A = 40 m2 Flift = 63,600 N P2 v2 http://www.grc.nasa.gov/WWW/K-12/airplane/foil2.html PHY 113 -- Lecture 16

  19. Peer instruction question • Suppose you see a tornado coming toward your house. Assuming that you have enough time, which of the following should you do before entering your shelter? • Open all of the windows and doors. • Make sure that all of the windows and doors are tightly shut. PHY 113 -- Lecture 16

  20. Homework problem: A hypodermic syringe contains a medicine with the density of water. The barrel of the syringe has a cross-sectional area A=2.5x10-5m2, and the needle has a cross-sectional area a= 1.0x10-8m2. In the absence of a force on the plunger, the pressure everywhere is 1 atm. A force F of magnitude 2 N acts on the plunger, making the medicine squirt horizontally from the needle. Determine the speed of the medicine as leave the needle’s tip. PHY 113 -- Lecture 16

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