1. PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 12

2. Newton’s Law of gravitation Kepler’s Laws of Planetary motion 1.Ellipses with sun at focus 2.Sweep out equal areas in equal times 3. Last Lecture

3. PE = mgh valid only near Earth’s surface For arbitrary altitude Zero reference level is at r=  Gravitational Potential Energy

4. Example 7.18 You wish to hurl a projectile from the surface of the Earth (R e = 6.38x10 6 m) to an altitude of 20x10 6 m above the surface of the Earth. Ignore rotation of the Earth and air resistance. a) What initial velocity is required? b) What velocity would be required in order for the projectile to reach infinitely high? I.e., what is the escape velocity? c) (skip) How does the escape velocity compare to the velocity required for a low earth orbit? a) 9,736 m/s b) 11,181 m/s c) 7,906 m/s

5. Chapter 8 Rotational Equilibrium and Rotational Dynamics

6. Wrench Demo

7. Torque Torque, , is tendency of a force to rotate object about some axis F is the force d is the lever arm (or moment arm) Units are Newton-meters Door Demo

8. Torque is vector quantity Direction determined by axis of twist Perpendicular to both r and F Clockwise torques point into paper. Defined as negative Counter-clockwise torques point out of paper. Defined as positive rr F F - +

9. Non-perpendicular forces Φ is the angle between F and r

10. Torque and Equilibrium Forces sum to zero (no linear motion) Torques sum to zero (no rotation)

11. Axis of Rotation Torques require point of reference Point can be anywhere Use same point for all torques Pick the point to make problem easiest (eliminate unwanted Forces from equation)

12. Example 8.1 Given M = 120 kg. Neglect the mass of the beam. a) Find the tension in the cable b) What is the force between the beam and the wall a) T=824 N b) f=353 N

13. Another Example Given: W=50 N, L=0.35 m, x=0.03 m Find the tension in the muscle F = 583 N x L W

14. Center of Gravity Gravitational force acts on all points of an extended object However, one can treat gravity as if it acts at one point: the center-of-gravity. Center of gravity:

15. Example 8.2 Given: x = 1.5 m, L = 5.0 m, w beam = 300 N, w man = 600 N Find: T x L T = 413 N

16. Example 8.3 Consider the 400-kg beam shown below. Find T R T R = 1 121 N

17. Example 8.4a Given: W beam =300 W box =200 Find: T left What point should I use for torque origin? ABCDABCD

18. Example 8.4b Given: T left =300 T right =500 Find: W beam What point should I use for torque origin? ABCDABCD

19. Example 8.4c Given: T left =250 T right =400 Find: W box What point should I use for torque origin? ABCDABCD

20. Example 8.4d Given: W beam =300 W box =200 Find: T right What point should I use for torque origin? ABCDABCD

21. Example 8.4e Given: T left =250 W beam =250 Find: W box What point should I use for torque origin? ABCDABCD

22. Torque and Angular Acceleration Analogous to relation between F and a Moment of Inertia m F R

23. Moment of inertia, I: rotational analog to mass r defined relative to rotation axis SI units are kg m 2

24. Baton Demo Moment-of-Inertia Demo

25. More About Moment of Inertia Depends on mass and its distribution. If mass is distributed further from axis of rotation, moment of inertia will be larger.

26. Moment of Inertia of a Uniform Ring Divide ring into segments The radius of each segment is R

27. Example 8.6 What is the moment of inertia of the following point masses arranged in a square? a) about the x-axis? b) about the y-axis? c) about the z-axis? a) 0.72 kg  m 2 b) 1.08 kg  m 2 c) 1.8 kg  m 2

28. Other Moments of Inertia

29. bicycle rim filled can of coke baton baseball bat basketball boulder

30. Example 8.7 Treat the spindle as a solid cylinder. a) What is the moment of Inertia of the spindle? (M=5.0 kg, R=0.6 m) b) If the tension in the rope is 10 N, what is the angular acceleration of the wheel? c) What is the acceleration of the bucket? d) What is the mass of the bucket? M a) 0.9 kg  m 2 b) 6.67 rad/s 2 c) 4 m/s 2 d) 1.72 kg

31. Example 8.9 A 600-kg solid cylinder of radius 0.6 m which can rotate freely about its axis is accelerated by hanging a 240 kg mass from the end by a string which is wrapped about the cylinder. a) Find the linear acceleration of the mass. b) What is the speed of the mass after it has dropped 2.5 m? 4.36 m/s 2 4.67 m/s