10 Rotational Motion and Angular Momentum

# 68 10.2 Kinematics of Rotational Motion

### Summary

• Observe the kinematics of rotational motion.
• Derive rotational kinematic equations.
• Evaluate problem solving strategies for rotational kinematics.

Just by using our intuition, we can begin to see how rotational quantities likeandare related to one another. For example, if a motorcycle wheel has a large angular acceleration for a fairly long time, it ends up spinning rapidly and rotates through many revolutions. In more technical terms, if the wheel’s angular accelerationis large for a long period of timethen the final angular velocityand angle of rotationare large. The wheel’s rotational motion is exactly analogous to the fact that the motorcycle’s large translational acceleration produces a large final velocity, and the distance traveled will also be large.

Kinematics is the description of motion. The kinematics of rotational motion describes the relationships among rotation angle, angular velocity, angular acceleration, and time. Let us start by finding an equation relatingandTo determine this equation, we recall a familiar kinematic equation for translational, or straight-line, motion:

Note that in rotational motionand we shall use the symbolfor tangential or linear acceleration from now on. As in linear kinematics, we assumeis constant, which means that angular accelerationis also a constant, becauseNow, let us substituteandinto the linear equation above:

The radiuscancels in the equation, yielding

whereis the initial angular velocity. This last equation is a kinematic relationship amongand—that is, it describes their relationship without reference to forces or masses that may affect rotation. It is also precisely analogous in form to its translational counterpart.

### MAKING CONNECTIONS

Kinematics for rotational motion is completely analogous to translational kinematics, first presented in Chapter 2 One-Dimensional Kinematics. Kinematics is concerned with the description of motion without regard to force or mass. We will find that translational kinematic quantities, such as displacement, velocity, and acceleration have direct analogs in rotational motion.

Starting with the four kinematic equations we developed in Chapter 2 One-Dimensional Kinematics, we can derive the following four rotational kinematic equations (presented together with their translational counterparts):

Rotational Translational
(constant)
(constant)
(constant)
Table 2. Rotational Kinematic Equations.

In these equations, the subscript 0 denotes initial values (andare initial values), and the average angular velocity and average velocityare defined as follows:

[latex size=”2″]\boldsymbol{\frac{\omega_0+\omega}{2}}[/latex][latex size=”2″]\boldsymbol{\frac{v_0+v}{2}}.[/latex]

The equations given above in Table 2 can be used to solve any rotational or translational kinematics problem in whichandare constant.

### PROBLEM-SOLVING STRATEGY FOR ROTATIONAL KINEMATICS

1. Examine the situation to determine that rotational kinematics (rotational motion) is involved. Rotation must be involved, but without the need to consider forces or masses that affect the motion.
2. Identify exactly what needs to be determined in the problem (identify the unknowns). A sketch of the situation is useful.
3. Make a list of what is given or can be inferred from the problem as stated (identify the knowns).
4. Solve the appropriate equation or equations for the quantity to be determined (the unknown). It can be useful to think in terms of a translational analog because by now you are familiar with such motion.
5. Substitute the known values along with their units into the appropriate equation, and obtain numerical solutions complete with units. Be sure to use units of radians for angles.
6. Check your answer to see if it is reasonable: Does your answer make sense?

### Example 1: Calculating the Acceleration of a Fishing Reel

A deep-sea fisherman hooks a big fish that swims away from the boat pulling the fishing line from his fishing reel. The whole system is initially at rest and the fishing line unwinds from the reel at a radius of 4.50 cm from its axis of rotation. The reel is given an angular acceleration offor 2.00 s as seen in Figure 1.

(a) What is the final angular velocity of the reel?

(b) At what speed is fishing line leaving the reel after 2.00 s elapses?

(c) How many revolutions does the reel make?

(d) How many meters of fishing line come off the reel in this time?

Strategy

In each part of this example, the strategy is the same as it was for solving problems in linear kinematics. In particular, known values are identified and a relationship is then sought that can be used to solve for the unknown.

Solution for (a)

Hereandare given andneeds to be determined. The most straightforward equation to use isbecause the unknown is already on one side and all other terms are known. That equation states that

We are also given that(it starts from rest), so that

Solution for (b)

Now thatis known, the speedcan most easily be found using the relationship

where the radiusof the reel is given to be 4.50 cm; thus,

Note again that radians must always be used in any calculation relating linear and angular quantities. Also, because radians are dimensionless, we have

Solution for (c)

Here, we are asked to find the number of revolutions. Becausewe can find the number of revolutions by findingin radians. We are givenandand we knowis zero, so thatcan be obtained using

Converting radians to revolutions gives

[latex size=”2″]\boldsymbol{\frac{1\textbf{ rev}}{2\pi\textbf{ rad}}}[/latex]

Solution for (d)

The number of meters of fishing line iswhich can be obtained through its relationship with

Discussion

This example illustrates that relationships among rotational quantities are highly analogous to those among linear quantities. We also see in this example how linear and rotational quantities are connected. The answers to the questions are realistic. After unwinding for two seconds, the reel is found to spin at 220 rad/s, which is 2100 rpm. (No wonder reels sometimes make high-pitched sounds.) The amount of fishing line played out is 9.90 m, about right for when the big fish bites.

### Example 2: Calculating the Duration When the Fishing Reel Slows Down and Stops

Now let us consider what happens if the fisherman applies a brake to the spinning reel, achieving an angular acceleration ofHow long does it take the reel to come to a stop?

Strategy

We are asked to find the timefor the reel to come to a stop. The initial and final conditions are different from those in the previous problem, which involved the same fishing reel. Now we see that the initial angular velocity isand the final angular velocityis zero. The angular acceleration is given to beExamining the available equations, we see all quantities but t are known inmaking it easiest to use this equation.

Solution

The equation states

We solve the equation algebraically for t, and then substitute the known values as usual, yielding

[latex size=”2″]\boldsymbol{\frac{\omega-\omega_0}{\alpha}}[/latex][latex size=”2″]\boldsymbol{\frac{0-220\textbf{ rad/s}}{-300\textbf{ rad/s}^2}}[/latex]

Discussion

Note that care must be taken with the signs that indicate the directions of various quantities. Also, note that the time to stop the reel is fairly small because the acceleration is rather large. Fishing lines sometimes snap because of the accelerations involved, and fishermen often let the fish swim for a while before applying brakes on the reel. A tired fish will be slower, requiring a smaller acceleration.

### Example 3: Calculating the Slow Acceleration of Trains and Their Wheels

Large freight trains accelerate very slowly. Suppose one such train accelerates from rest, giving its 0.350-m-radius wheels an angular acceleration ofAfter the wheels have made 200 revolutions (assume no slippage): (a) How far has the train moved down the track? (b) What are the final angular velocity of the wheels and the linear velocity of the train?

Strategy

In part (a), we are asked to findand in (b) we are asked to findandWe are given the number of revolutionsthe radius of the wheelsand the angular acceleration

Solution for (a)

The distanceis very easily found from the relationship between distance and rotation angle:

[latex size=”2″]\boldsymbol{\frac{x}{r}}.[/latex]

Solving this equation foryields

Before using this equation, we must convert the number of revolutions into radians, because we are dealing with a relationship between linear and rotational quantities:

[latex size=”2″]\boldsymbol{\frac{2\pi\textbf{rad}}{1\textbf{ rev}}}[/latex]

Now we can substitute the known values intoto find the distance the train moved down the track:

Solution for (b)

We cannot use any equation that incorporatesto findbecause the equation would have at least two unknown values. The equationwill work, because we know the values for all variables except

Taking the square root of this equation and entering the known values gives

We can find the linear velocity of the train,through its relationship to

Discussion

The distance traveled is fairly large and the final velocity is fairly slow (just under 32 km/h).

There is translational motion even for something spinning in place, as the following example illustrates. Figure 2 shows a fly on the edge of a rotating microwave oven plate. The example below calculates the total distance it travels.

### Example 4: Calculating the Distance Traveled by a Fly on the Edge of a Microwave Oven Plate

A person decides to use a microwave oven to reheat some lunch. In the process, a fly accidentally flies into the microwave and lands on the outer edge of the rotating plate and remains there. If the plate has a radius of 0.15 m and rotates at 6.0 rpm, calculate the total distance traveled by the fly during a 2.0-min cooking period. (Ignore the start-up and slow-down times.)

Strategy

First, find the total number of revolutionsand then the linear distancetraveled.can be used to findbecauseis given to be 6.0 rpm.

Solution

Entering known values intogives

As always, it is necessary to convert revolutions to radians before calculating a linear quantity likefrom an angular quantity like

[latex size=”2″]\boldsymbol{\frac{2\pi\textbf{ rad}}{1\textbf{ rev}}}[/latex]

Now, using the relationship betweenandwe can determine the distance traveled:

Discussion

Quite a trip (if it survives)! Note that this distance is the total distance traveled by the fly. Displacement is actually zero for complete revolutions because they bring the fly back to its original position. The distinction between total distance traveled and displacement was first noted in Chapter 2 One-Dimensional Kinematics.

### Check Your Understanding

1: Rotational kinematics has many useful relationships, often expressed in equation form. Are these relationships laws of physics or are they simply descriptive? (Hint: the same question applies to linear kinematics.)

# Section Summary

• Kinematics is the description of motion.
• The kinematics of rotational motion describes the relationships among rotation angle, angular velocity, angular acceleration, and time.
• Starting with the four kinematic equations we developed in the Chapter 2 One-Dimensional Kinematics, we can derive the four rotational kinematic equations (presented together with their translational counterparts) seen in Table 2.
• In these equations, the subscript 0 denotes initial values (andare initial values), and the average angular velocityand average velocityare defined as follows:
[latex size=”2″]\boldsymbol{\frac{\omega_0+\omega}{2}}[/latex][latex size=”2″]\boldsymbol{\frac{v_0+v}{2}}.[/latex]

### Problems & Exercises

1: With the aid of a string, a gyroscope is accelerated from rest to 32 rad/s in 0.40 s.

(a) What is its angular acceleration in rad/s2?

(b) How many revolutions does it go through in the process?

2: Suppose a piece of dust finds itself on a CD. If the spin rate of the CD is 500 rpm, and the piece of dust is 4.3 cm from the center, what is the total distance traveled by the dust in 3 minutes? (Ignore accelerations due to getting the CD rotating.)

3: A gyroscope slows from an initial rate of 32.0 rad/s at a rate of

(a) How long does it take to come to rest?

(b) How many revolutions does it make before stopping?

4: During a very quick stop, a car decelerates at

(a) What is the angular acceleration of its 0.280-m-radius tires, assuming they do not slip on the pavement?

(b) How many revolutions do the tires make before coming to rest, given their initial angular velocity is?

(c) How long does the car take to stop completely?

(d) What distance does the car travel in this time?

(e) What was the car’s initial velocity?

(f) Do the values obtained seem reasonable, considering that this stop happens very quickly?

5: Everyday application: Suppose a yo-yo has a center shaft that has a 0.250 cm radius and that its string is being pulled.

(a) If the string is stationary and the yo-yo accelerates away from it at a rate ofwhat is the angular acceleration of the yo-yo?

(b) What is the angular velocity after 0.750 s if it starts from rest?

(c) The outside radius of the yo-yo is 3.50 cm. What is the tangential acceleration of a point on its edge?

## Glossary

kinematics of rotational motion
describes the relationships among rotation angle, angular velocity, angular acceleration, and time

### Solutions

Check Your Understanding

1: Rotational kinematics (just like linear kinematics) is descriptive and does not represent laws of nature. With kinematics, we can describe many things to great precision but kinematics does not consider causes. For example, a large angular acceleration describes a very rapid change in angular velocity without any consideration of its cause.

Problems & Exercises

1:

(a)

(b) 1.0 rev

3:

(a) 45.7 s

(b) 116 rev

5:

a)

b) 450 rad/s

c) 21.0 m/s

## License

10.2 Kinematics of Rotational Motion by OpenStax is licensed under a Creative Commons Attribution 4.0 International License, except where otherwise noted.