1. Chapter 8 Rotational Equilibrium and Rotational Dynamics

2. Fig 8.1, p.221 Slide 1

3. Torque Torque,, is the tendency of a force to rotate an object about some axis Torque,, is the tendency of a force to rotate an object about some axis is the torque is the torque –symbol is the Greek tau F is the force F is the force d is the lever arm (or moment arm) d is the lever arm (or moment arm)

4. Lever Arm The lever arm, d, is the perpendicular distance from the axis of rotation to a line drawn from the axis of rotation to a line drawn along the the direction of the force The lever arm, d, is the perpendicular distance from the axis of rotation to a line drawn from the axis of rotation to a line drawn along the the direction of the force d = L sin Φ d = L sin Φ

5. An Alternative Look at Torque The force could also be resolved into its x- and y- components The force could also be resolved into its x- and y- components The x-component, F cos Φ, produces 0 torque The x-component, F cos Φ, produces 0 torque The y-component, F sin Φ, produces a non-zero torque The y-component, F sin Φ, produces a non-zero torque

6. Torque and Equilibrium First Condition of Equilibrium First Condition of Equilibrium This is a statement of translational equilibrium This is a statement of translational equilibrium To ensure mechanical equilibrium, you need to ensure rotational equilibrium as well as translational To ensure mechanical equilibrium, you need to ensure rotational equilibrium as well as translational The Second Condition of Equilibrium states The Second Condition of Equilibrium states The net external torque must be zero The net external torque must be zero

7. Mechanical Equilibrium In this case, the First Condition of Equilibrium is satisfied In this case, the First Condition of Equilibrium is satisfied The Second Condition is not satisfied The Second Condition is not satisfied Both forces would produce clockwise rotations Both forces would produce clockwise rotations

8. Fig 8.12a, p.228 Slide 17 If the object is in equilibrium, it does not matter where you put the axis of rotation for calculating the net torque.If the object is in equilibrium, it does not matter where you put the axis of rotation for calculating the net torque. When solving a problem, you must specify an axis of rotation and maintain that choice consistently throughout the problem.When solving a problem, you must specify an axis of rotation and maintain that choice consistently throughout the problem.

9. Fig 8.12bc, p.228 Slide 18

10. Torque and Angular Acceleration An object that rotates at uniform angular velocity has zero net torque acting on it An object that rotates at uniform angular velocity has zero net torque acting on it When a rigid object is subject to a net torque, it has an angular acceleration When a rigid object is subject to a net torque, it has an angular acceleration The angular acceleration is directly proportional to the net torque The angular acceleration is directly proportional to the net torque The relationship is analogous to Newton’s Second Law ∑F = ma The relationship is analogous to Newton’s Second Law ∑F = ma

11. Moment of Inertia The rotational analog of mass is called the moment of inertia, I, of the object The rotational analog of mass is called the moment of inertia, I, of the object (SI units are kg m 2) (SI units are kg m 2) angular acceleration is directly proportional to the net torque angular acceleration is directly proportional to the net torque angular acceleration is inversely proportional to the moment of inertia of the object angular acceleration is inversely proportional to the moment of inertia of the object **The moment of inertia depends upon the location of the axis of rotation

12. Moment of Inertia of a Uniform Ring Image the hoop is divided into a number of small segments, m 1 … Image the hoop is divided into a number of small segments, m 1 … These segments are equidistant from the axis These segments are equidistant from the axis

13. Other Moments of Inertia

14. Angular Momentum Like relationship between force and momentum in a linear system, we can a relationship between torque and angular momentum Like relationship between force and momentum in a linear system, we can a relationship between torque and angular momentum Angular momentum is defined as Angular momentum is defined as L = I ω L = I ω and and If the net torque is zero, the angular momentum remains constant If the net torque is zero, the angular momentum remains constant

15. Fig 8.29, p.240 Slide 38

16. Fig P8.55, p.252 Slide 70

17. Coordinates of the Center of Gravity The coordinates of the center of gravity can be found from the sum of the torques acting on the individual particles being set equal to the torque produced by the weight of the object The coordinates of the center of gravity can be found from the sum of the torques acting on the individual particles being set equal to the torque produced by the weight of the object Example – uniform ruler Example – uniform ruler

18. Experimentally Determining the Center of Gravity The wrench is hung freely from two different pivots The wrench is hung freely from two different pivots The intersection of the lines indicates the center of gravity The intersection of the lines indicates the center of gravity A rigid object can be balanced by a single force equal in magnitude to its weight as long as the force is acting upward through the object’s center of gravity A rigid object can be balanced by a single force equal in magnitude to its weight as long as the force is acting upward through the object’s center of gravity

19. Fig UN8.1, p.224 Slide 8

20. Fig P8.64, p.253 Slide 75 =41.8°

21. Example of a Free Body Diagram Isolate the object to be analyzed Isolate the object to be analyzed Draw the free body diagram for that object Draw the free body diagram for that object Include all the external forces acting on the object Include all the external forces acting on the object

22. Rotational Kinetic Energy An object rotating about some axis with an angular speed, ω, has rotational kinetic energy ½Iω 2 An object rotating about some axis with an angular speed, ω, has rotational kinetic energy ½Iω 2 Energy concepts can be useful for simplifying the analysis of rotational motion Energy concepts can be useful for simplifying the analysis of rotational motion

23. Total Energy of a System Conservation of Mechanical Energy Conservation of Mechanical Energy Remember, this is for conservative forces, no dissipative forces such as friction can be present Remember, this is for conservative forces, no dissipative forces such as friction can be present

24. Fig 8.25, p.236 Slide 36

25. Fig P8.43, p.250 Slide 66

26. Fig 8.14, p.229 Slide 25