1. Review Chap. 10 Dynamics of Rotational Motion
PHYS 218 sec
Review
Chap. 10
Dynamics of Rotational Motion

2. What you have to know Dynamics of rotational motion Torque
Equation of motion for a rotational motion
Rotation about a moving axis
Work & power
Angular momentum and its conservation

3. Translational motion: governed by forces
Torque
Translational motion: governed by forces
Rotational motion: governed by torques
When you define a rotational motion, you should specify the axis of rotation. Therefore, physical quantities in rotational motion must include information about the location of the axis of rotation.
This makes the definitions of those physical quantities include x or r.
For example, even if the same force (same magnitude & same direction) is applied, the rotational motion depends on where the force exerts on, i.e., the distance between the axis of ration and the point where the force exerts on.
When you have a rotational motion, determine whether the rotation is clockwise or counterclockwise.

4. This force causes counterclockwise rotation. (So, t is positive)
Torque
definition
This force causes counterclockwise rotation. (So, t is positive)
Axis of rotation

5. Line of action of the force F
Torque
Line of action of the force F
Lever arm
Only the tangential force can give a torque.

6. Note the similarity of the two equations.
Torque for a rigid body
Note the similarity of the two equations.
Rotational analog of Newton’s 2nd law for a rigid body

7. Reproduce the result of Ex 9.8 as explained in the class
Same situation as in Ex 9.8
Free-body diagram
Reproduce the result of Ex 9.8
as explained in the class
Direction of the rotation & sing of the torque

8. Ex 10.3
Same situation as in Ex 9.9
Free-body diagram
cylinder
block
Obtain v !

9. Rigid-body rotation about a moving axis
Extend the analysis to the case where the axis of rotation moves
Translation + Rotation cm

11. Rolling without slipping

12. Translation + Rotation
For translation, concentrate the mass of the object on its CM g same as the motion of a point-like particle
For rotation, consider the rotation about CM g same as the rotational motion when the CM is fixed.
The second equation is valid, if
The axis through the CM must be an axis of symmetry
The axis must not change direction

13. Speed of a primitive yo-yo
Ex 10.4
Speed of a primitive yo-yo
initial
final

14. Race of the rolling bodies
Ex 10.5
Race of the rolling bodies

15. Acceleration of a primitive yo-yo (cf. Ex 10.4)
Rolling without slipping
Try to reproduce the result of Ex 10.4

16. Solid bowling ball (rolling without slipping)
Ex 10.7
Solid bowling ball (rolling without slipping)
Free-body diagram
If b is small, the friction force which is required to have the rolling is small.
If b is large, the ball easily slips, then we need a large friction force to make it roll.

17. Work & Power in rotational motion
To rotate a body, a force should be applied. Then this force do work on it.

18. Work –energy theorem

19. Similarly, we define angular momentum L
(linear) momentum p
Similarly, we define angular momentum L
This is defined with r, so it depends on the choice of the origin.
This is a vector product. Therefore, the angular momentum is perpendicular to the plane spanned by r and p. If r and p lie on the xy-plane, L is in the z-direction.
This is always true.

20. Note the similarity.

21. Angular momentum of a rigid-body
This is valid if the rigid-body lies on the xy-plane.

22. Angular momentum of a rigid-body

23. Angular momentum of a rigid-body

25. Conservation of angular momentum

26. Collision problem including rotational motion.
Ex 10.14
Collision problem including rotational motion.
g use angular momentum conservation d
after
before
Use the numbers given in the textbook to verify the result.
Also check the change in kinetic energies.

27. Gyroscopes & precession
The motion of gyroscope was discussed in the class.
Here I do not repeat it.
But you should understand that the gyroscope has precession and this is due to the vector nature of angular momentum.