1. Rotational Equilibrium and Rotational Dynamics
Chapter 8
Rotational Equilibrium
and
Rotational Dynamics

2. Force vs. Torque Forces cause accelerations
Torques cause angular accelerations
Force and torque are related

3. Torque The door is free to rotate about an axis through O
There are three factors that determine the effectiveness of the force in opening the door:
The magnitude of the force
The position of the application of the force
The angle at which the force is applied

4. Torque, cont
Torque, t, is the tendency of a force to rotate an object about some axis
t = r F
t is the torque
symbol is the Greek tau
F is the force
r is the length of the position vector
SI unit is N.m

5. Direction of Torque Torque is a vector quantity
The direction is perpendicular to the plane determined by the position vector and the force
If the turning tendency of the force is counterclockwise, the torque will be positive
If the turning tendency is clockwise, the torque will be negative

6. Multiple Torques
When two or more torques are acting on an object, the torques are added
As vectors
If the net torque is zero, the object’s rate of rotation doesn’t change

7. General Definition of Torque
The applied force is not always perpendicular to the position vector
The component of the force perpendicular to the object will cause it to rotate

8. General Definition of Torque, cont
When the force is parallel to the position vector, no rotation occurs
When the force is at some angle, the perpendicular component causes the rotation

9. General Definition of Torque, final
Taking the angle into account leads to a more general definition of torque:
t = r F sin q
F is the force
r is the position vector
q is the angle between the force and the position vector

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

11. Net Torque
The net torque is the sum of all the torques produced by all the forces
Remember to account for the direction of the tendency for rotation
Counterclockwise torques are positive
Clockwise torques are negative

12. Example 1
If the torque required to loosen a nut that is holding a flat tire in place on a car has a magnitude of 40.0 N ∙ m, what minimum force must be exerted by the mechanic at the end of a 30.0-cm lug wrench to accomplish the task?

13. Torque and Equilibrium
First Condition of Equilibrium
The net external force must be zero
This is a necessary, but not sufficient, condition to ensure that an object is in complete mechanical equilibrium
This is a statement of translational equilibrium

14. Torque and Equilibrium, cont
To ensure mechanical equilibrium, you need to ensure rotational equilibrium as well as translational
The Second Condition of Equilibrium states
The net external torque must be zero

15. Equilibrium Example
The woman, mass m, sits on the left end of the see-saw
The man, mass M, sits where the see-saw will be balanced
Apply the Second Condition of Equilibrium and solve for the unknown distance, x

16. Axis of Rotation
If the object is in equilibrium, it does not matter where you put the axis of rotation for calculating the net torque
The location of the axis of rotation is completely arbitrary
Often the nature of the problem will suggest a convenient location for the axis
When solving a problem, you must specify an axis of rotation
Once you have chosen an axis, you must maintain that choice consistently throughout the problem

17. Center of Gravity
The force of gravity acting on an object must be considered
In finding the torque produced by the force of gravity, all of the weight of the object can be considered to be concentrated at a single point

18. Calculating the Center of Gravity
The object is divided up into a large number of very small particles of weight (mg)
Each particle will have a set of coordinates indicating its location (x,y)

19. Calculating the Center of Gravity, cont.
We assume the object is free to rotate about its center
The torque produced by each particle about the axis of rotation is equal to its weight times its lever arm
For example, t1 = m1 g x1

20. Calculating the Center of Gravity, cont.
We wish to locate the point of application of the single force whose magnitude is equal to the weight of the object, and whose effect on the rotation is the same as all the individual particles.
This point is called the center of gravity of the object

21. 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

22. Center of Gravity of a Uniform Object
The center of gravity of a homogenous, symmetric body must lie on the axis of symmetry.
Often, the center of gravity of such an object is the geometric center of the object.

23. Experimentally Determining the Center of Gravity
The wrench is hung freely from two different pivots
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

24. Notes About Equilibrium
A zero net torque does not mean the absence of rotational motion
An object that rotates at uniform angular velocity can be under the influence of a zero net torque
This is analogous to the translational situation where a zero net force does not mean the object is not in motion

25. Solving Equilibrium Problems
Draw a diagram of the system
Include coordinates and choose a rotation axis
Isolate the object being analyzed and draw a free body diagram showing all the external forces acting on the object
For systems containing more than one object, draw a separate free body diagram for each object

26. Problem Solving, cont. Apply the Second Condition of Equilibrium
This will yield a single equation, often with one unknown which can be solved immediately
Apply the First Condition of Equilibrium
This will give you two more equations
Solve the resulting simultaneous equations for all of the unknowns
Solving by substitution is generally easiest

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

28. Example of a Free Body Diagram (Beam)
The free body diagram includes the directions of the forces
The weights act through the centers of gravity of their objects

29. Example 2
Write the necessary equations of equilibrium of the object shown in Figure P8.4. Take the origin of the torque equation about an axis perpendicular to the page through the point O.

30. Example 3
A meterstick is found to balance at the 49.7-cm mark when placed on a fulcrum. When a 50.0-gram mass is attached at the 10.0-cm mark, the fulcrum must be moved to the 39.2-cm mark for balance. What is the mass of the meter stick?

31. Example 4
A window washer is standing on a scaffold supported by a vertical rope at each end. The scaffold weighs 200 N and is 3.00 m long. What is the tension in each rope when the 700-N worker stands 1.00 m from one end?

32. Example 5
A 500-N uniform rectangular sign 4.00 m wide and 3.00 m high is suspended from a horizontal, 6.00-m-long, uniform, 100-N rod as indicated in Figure P8.17. The left end of the rod is supported by a hinge, and the right end is supported by a thin cable making a 30.0° angle with the vertical. (a) Find the tension T in the cable. (b) Find the horizontal and vertical components of force exerted on the left end of the rod by the hinge.

33. Torque and Angular Acceleration
When a rigid object is subject to a net torque (≠0), it undergoes an angular acceleration
The angular acceleration is directly proportional to the net torque
The relationship is analogous to ∑F = ma
Newton’s Second Law

34. Moment of Inertia
The angular acceleration is inversely proportional to the analogy of the mass in a rotating system
This mass analog is called the moment of inertia, I, of the object
SI units are kg m2

35. Newton’s Second Law for a Rotating Object
The angular acceleration is directly proportional to the net torque
The angular acceleration is inversely proportional to the moment of inertia of the object

36. More About Moment of Inertia
There is a major difference between moment of inertia and mass: the moment of inertia depends on the quantity of matter and its distribution in the rigid object.
The moment of inertia also depends upon the location of the axis of rotation

37. Moment of Inertia of a Uniform Ring
Image the hoop is divided into a number of small segments, m1 …
These segments are equidistant from the axis

38. Other Moments of Inertia

39. Example, Newton’s Second Law for Rotation
Draw free body diagrams of each object
Only the cylinder is rotating, so apply St = I a
The bucket is falling, but not rotating, so apply SF = m a
Remember that a = a r and solve the resulting equations

40. Example 6
A potter’s wheel having a radius of 0.50 m and a moment of inertia of 12 kg ∙ m2 is rotating freely at 50 rev/min. The potter can stop the wheel in 6.0 s by pressing a wet rag against the rim and exerting a radially inward force of 70 N. Find the effective coefficient of kinetic friction between the wheel and the wet rag.

41. Example 7
A 150-kg merry-go-round in the shape of a uniform, solid, horizontal disk of radius 1.50 m is set in motion by wrapping a rope about the rim of the disk and pulling on the rope. What constant force must be exerted on the rope to bring the merry-go-round from rest to an angular speed of rev/s in 2.00 s?

42. Rotational Kinetic Energy
An object rotating about some axis with an angular speed, ω, has rotational kinetic energy ½Iω2
Energy concepts can be useful for simplifying the analysis of rotational motion

43. Total Energy of a System
Conservation of Mechanical Energy
Remember, this is for conservative forces, no dissipative forces such as friction can be present
Potential energies of any other conservative forces could be added

44. Work-Energy in a Rotating System
In the case where there are dissipative forces such as friction, use the generalized Work-Energy Theorem instead of Conservation of Energy
Wnc = DKEt + DKER + DPE

45. General Problem Solving Hints
The same basic techniques that were used in linear motion can be applied to rotational motion.
Analogies: F becomes , m becomes I and a becomes , v becomes ω and x becomes θ

46. Problem Solving Hints for Energy Methods
Choose two points of interest
One where all the necessary information is given
The other where information is desired
Identify the conservative and nonconservative forces

47. Problem Solving Hints for Energy Methods, cont
Write the general equation for the Work-Energy theorem if there are nonconservative forces
Use Conservation of Energy if there are no nonconservative forces
Use v = w to combine terms
Solve for the unknown

48. Example 8
A 10.0-kg cylinder rolls without slipping on a rough surface. At an instant when its center of gravity has a speed of 10.0 m/s, determine (a) the translational kinetic energy of its center of gravity, (b) the rotational kinetic energy about its center of gravity, and (c) its total kinetic energy.

49. Angular Momentum
Similarly to the relationship between force and momentum in a linear system, we can show the relationship between torque and angular momentum
Angular momentum is defined as
L = I ω
and

50. Angular Momentum, cont
If the net torque is zero, the angular momentum remains constant
Conservation of Angular Momentum states: The angular momentum of a system is conserved when the net external torque acting on the systems is zero.
That is, when

51. Conservation Rules, Summary
In an isolated system, the following quantities are conserved:
Mechanical energy
Linear momentum
Angular momentum

52. Conservation of Angular Momentum, Example
With hands and feet drawn closer to the body, the skater’s angular speed increases
L is conserved, I decreases, w increases

53. Example 9
A 60.0-kg woman stands at the rim of a horizontal turntable having a moment of inertia of 500 kg ∙ m2 and a radius of 2.00 m. The turntable is initially at rest and is free to rotate about a frictionless, vertical axle through its center. The woman then starts walking around the rim clockwise (as viewed from above the system) at a constant speed of 1.50 m/s relative to the Earth. (a) In what direction and with what angular speed does the turntable rotate? (b) How much work does the woman do to set herself and the turntable into motion?

54. Example 10
A light rigid rod 1.00 m in length rotates about an axis perpendicular to its length and through its center, as shown in Figure P8.45. Two particles of masses 4.00 kg and 3.00 kg are connected to the ends of the rod. What is the angular momentum of the system if the speed of each particle is 5.00 m/s? (Neglect the rod’s mass.)