1. ROTATIONAL MOTION
Y. Edi Gunanto

2. Gerak Rotasi Dalam Fisika dibedakan 2 jenis gerak benda :
1. Gerak Translasi :
the motion of an object through space. (change of location)
2. Gerak Rotasi :
the spinning of an object around an axis. (change of orientation)

3. Objects may have purely translational motion, purely rotational motion, or both.
A rigid body (benda tegar) is composed of particles in fixed positions.
In a rigid body undergoing purely rotational motion, all points of the body move in circles centered around a line called the axis of rotation.

4. Key to learning rotational motion:
THE CONCEPTS FROM TRANSLATIONAL MECHANICS (E.G. VELOCITY, ACCELERATION, FORCE ENERGY, & MOMENTUM) HAVE ANALOGOUS ROTATIONAL CONCEPTS.

5. Rotational Kinematics
Angular displacement () is the rotational analog of displacement (∆x). 

6. For one complete revolution:  = 2r/r = 2 radians So, 2 rad = 360°
Angular displacements are measured in radians.
 = Arc length/radius
 = r/r = 1 radian r  r
For one complete revolution:
 = 2r/r = 2 radians
So, 2 rad = 360°
 = 1 rad

7. l = Rq

8. Rotational Kinematics
Find the following:
 rad = ___ degrees
90° = ___ rad
1 rad = ___ degrees
10 rev = ___ rad
Answers
180
/2
57.3
20

9. Rotational Kinematics
Average angular velocity (avg) is the rotational analog of velocity (v).
Velocity = Displacement / Time
v = ∆x / t
Ang. velocity = Ang. displacement / Time
avg =  / t

10. Rotational Kinematics
What is the angular velocity of the points on a record rotating at 45 rpm?
 = 45 rev x (2 rad / 1 rev) = 90 rad
 =  / t
 = 90 rad / 60 s
 = 3/2 rad/s

11. Rotational Kinematics
Angular acceleration () is the rotational analog of acceleration (a).
Acceleration = Change in velocity / Time
a = ∆v / t
Ang. accel. = Change in Ang.veloc. / Time
 =  / t

12. Rotational Kinematics
A record begins spinning from rest and reaches a rotation of 45 rpm in three seconds. What is the angular acceleration of the points on the record?
 =  / t
 = (3/2 rad/s - 0) / 3 s
 = /2 rad/s2

13. Rotational Kinematics
Linear Motion
v = vo + at
∆x = (1/2)(vo + v)t
vavg = (1/2)(vo + v)
∆x = vot + (1/2)at2
v2 = vo2 + 2a∆x
Rotational Motion
= o + t
= (1/2)(o + )t
avg = (1/2)(o + )
= ot + (1/2)t2
2 = o2 + 2

14. Problem 1
Find:
ω at t = 0.30 s?
Angle PQ makes with x – axis at this time?
Given: ω = 27.5 rad/s at t = 0
α = -10 rad/s2
Line PQ lies on the disc along the x- axis

15. EXAMPLE 1 In addition to stated givens we know Θi= 0° at t = 0s
Given: ω = 27.5 rad/s at t = 0
α = -10 rad/s2
Line PG lies on the disc
along the x -axis
Part a Solution:
Use: ωz = ωiz + αzt for t = 0.3 s
ωz = (27.5 rad/s) + (-10 rad/s2)(0.3s)
= 24.5 rad/s

16. Part b In addition to stated givens we know Θi= 0° at t = 0s
Part b Solution:
Use: Θ = Θi + ωizt + ½ αzt for t = 0.3 s
Θ = 0 + (27.5 rad/s)(0.3s) + ½ (-10 rad/s2)(0.3s)2 = rad
# revolutions?: 7.8 rad (1rev/2π rad) = 1.24 rev
The disc has gone through one revolution plus 0.24 into the next. So the angle at that time with the x –axis is:
0.24 (360°/rev) = 87°

17. Rolling Motion (without slipping)
Rolling without slipping depends on static friction between the wheel, ball, etc. and the ground.
The friction is static because the rolling object’s point of contact with the ground is at rest at each moment.
Kinetic friction comes in if the object skids, that is, slides.
VERY IMPORTANT CONCEPT!

18. Rolling Without Slipping Involves Both Rotation and Translation.
Reference frame attached to ground
Static friction: wheel does not slide
Center of mass (CM)
Reference frame attached to wheel

19. Reference frame attached to the ground

20. Reference frame attached to the wheel

22. Torque
Torque (t ) deals with the dynamics, or causes of rotational motion.
Dynamics in linear motion dealt with force.
In rotational motion TORQUE is analogous to FORCE in linear motion.
That is, force through a distance
F t

23. t = RF = RFsinq t = R x F = RFsinq Definition of torque (magnitude)*
* Torque is a vector.
t = R x F = RFsinq

25. These two methods of calculation are completely equivalent.

26. Example 2 Torque on a compound wheel.
Two thin cylindrical wheels, of radii R1 = 30 cm and R2 = 50 cm, are attached to each other. Calculate the net torque on the two-wheel system due to the two forces shown, each of magnitude 50 N.

28. F2

29. Rotational Dynamics; Torque and Rotational Inertia
Linear Acceleration:
directly proportional to force.
inversely proportional to inertia.
Angular Acceleration:
directly proportional to torque.
inversely proportional to the moment of inertia.

30. Torque and Force
Moment of inertia
St = Ia
SF = ma

31. Example 3 Two Weights on a Bar: Different Axis, Different I.
Two small “weights” of mass 5.0 kg and 7.0 kg are mounted 4.0 m apart on a light rod (whose mass can be ignored). Calculate the moment of inertia of the system (a) when rotated about an axis half way between the weights, and (b) when the system rotates about an axis 0.50 m to the left of the 5.0 kg mass.

35. Example 4
A heavy pulley.
A 15.0-N force (represented by FT) is applied to a cord wrapped around a pulley of mass M = 4.0 kg and radius Ro = 33.0 cm. The pulley is observed to accelerate uniformly from rest to reach an angular speed of 30.0 rad/s. If there is a frictional torque (at the axle), t = 1.10 mN, determine the moment of inertia of the pulley. The pulley is assumed to rotate about its center.

37. Example 5
Rotating rod.
A uniform rod of mass M and length l can pivot freely (i.e., we ignore friction) about a hinge or pin attached to the case of a large machine. The rod is held horizontally and then released. At the moment of release determine (a) the angular acceleration of the rod (b) the linear acceleration of the tip of the rod. Assume the force of gravity acts at the CM of the rod.

39. Determining Moments of Inertia
The are two methods of determining moments of inertia:
By experiment (See Example 4)
By calculus

40. Using Calculus
For many bodies, or systems of particles, the moment of inertia can be calculated directly, as in Example 3.
Many bodies can be considered as a continuous distribution of mass. In this case we can write:
I = R2 dm
where dm represents the mass of an infinitesimal particle of the body and R is the perpendicular distance of the particle from the axis of rotation.

41. EXAMPLE 6 Show that the moment of inertia of a uniform rod length L :
a. throught the centre of mass
b. throught the end of rod

42. The Parallel-Axis and Perpendicular-Axis Theorems
Parallel-Axis Theorem: if the moment of inertia I is the moment of inertia of a body of total mass M about any axis, and ICM is the moment of inertia about an axis passing through the center of mass and parallel to the first axis but a distance h away, then
I = ICM + Mh2

43. Angular Momentum and Its Conservation
The SI units for L are kg.m2/s.
Linear momentum: p = mv
Angular momentum: L = Iw

44. Angular and Linear Momentum
dL dt
St = Ia =
dp dt
SF = ma =

45. Conservation of Angular Momentum
Law of Conservation of Angular Momentum
The total angular momentum of a rotating body remains constant if the net external torque acting on it is zero.
When there is zero net torque acting on a body, and the body is rotating about a fixed axis or about an axis through its CM such that the direction doesn’t change, we can write
Iw = Iowo = constant

46. When the skater pulls her arms in, she is decreasing her moment of inertia.

47. Example 7
Clutch design.
You are designing a clutch assembly for a piece of machinery. The clutch assembly consists of two cylindrical plates, of mass MA = 6.0 kg and MB = 9.0 kg, with equal radii Ro = 0.60 m. They are initially separated. Plate MA is accelerated from rest to an angular velocity w1 = 7.2 rad/s in a time Δt = 2.0 s. Calculate (a) the angular momentum of MA, and (b) the torque required to have accelerated MA from rest to w1.

48. Clutch design (cont.).
Next, plate MB, initially at rest but free to rotate without friction, is allowed to fall vertically so it is in firm contact with plate MA. Before contact, MA was rotating at constant w1, with no friction or other torque exerted on it. Upon contact, the two plates both rotate at a constant angular velocity w2, which is considerably less than w1. (c) Why does this happen, and what is w2?

50. Rotational Kinetic Energy
Linear Kinetic Energy: K = ½ mv2
Rotational Kinetic Energy: K = ½ Iw2

51. Work Linear work: W = ½ mv22 – ½ mv12 = ΔK
Rotational Work: Wrot = ½ Iw22 – ½ Iw12 = ΔKrot

52. Example 8
Rotating rod.
A rod of mass M is pivoted on a frictionless hinge at one end. The rod is held at rest horizontally and then released. Determine the angular velocity of the rod when it reaches the vertical position, and the speed of the rod’s tip at this moment.

54. Rotational Plus Translational Motion

55. Kinetic Energy = KCM + Krot
The Equations
Kinetic Energy = KCM + Krot
K = ½ MvCM + ½ ICMw2 2

56. Example 9 Sphere rolling down an incline.
What will be the speed of a solid sphere of mass M and radius Ro when it reaches the bottom of an incline if it starts from rest at a vertical height H and rolls without slipping? Compare to the result of sliding down the incline.

58. TERIMA KASIH