### Learning Objectives

By the end of this section, you will be able to:

- Define and distinguish between instantaneous acceleration and average acceleration.
- Calculate acceleration given initial time, initial velocity, final time, and final velocity.

The information presented in this section supports the following AP® learning objectives and science practices:

**3.A.1.1**The student is able to express the motion of an object using narrative, mathematical, and graphical representations.**(S.P. 1.5, 2.1, 2.2)****3.A.1.3**The student is able to analyze experimental data describing the motion of an object and is able to express the results of the analysis using narrative, mathematical, and graphical representations.**(S.P. 5.1)**

In everyday conversation, to accelerate means to speed up. The accelerator in a car can in fact cause it to speed up. The greater the acceleration, the greater the change in velocity over a given time. The formal definition of acceleration is consistent with these notions, but more inclusive.

### Average Acceleration

Average Acceleration is *the rate at which velocity changes*,

where *$\stackrel{-}{a}$* is average acceleration, *$v$* is velocity, and *$t$* is time. (The bar over the $a$ means *average* acceleration.)

Because acceleration is velocity in m/s divided by time in s, the SI units for acceleration are ${\text{m/s}}^{2}$, meters per second squared or meters per second per second, which literally means by how many meters per second the velocity changes every second.

Recall that velocity is a vector—it has both magnitude and direction. This means that a change in velocity can be a change in magnitude (or speed), but it can also be a change in *direction*. For example, if a car turns a corner at constant speed, it is accelerating because its direction is changing. The quicker you turn, the greater the acceleration. So there is an acceleration when velocity changes either in magnitude (an increase or decrease in speed) or in direction, or both.

### Acceleration as a Vector

Acceleration is a vector in the same direction as the *change* in velocity, $\mathrm{\Delta}v$. Since velocity is a vector, it can change either in magnitude or in direction. Acceleration is therefore a change in either speed or direction, or both.

Keep in mind that although acceleration is in the direction of the *change* in velocity, it is not always in the direction of *motion*. When an object's acceleration is in the same direction of its motion, the object will speed up. However, when an object's acceleration is opposite to the direction of its motion, the object will slow down. Speeding up and slowing down should not be confused with a positive and negative acceleration. The next two examples should help to make this distinction clear.

### Making Connections: Car Motion

Consider the acceleration and velocity of each car in terms of its direction of travel.

Because the positive direction is considered to the right of the paper, Car A is moving with a positive velocity. Because it is speeding up while moving with a positive velocity, its acceleration is also considered positive.

Because the positive direction is considered to the right of the paper, Car B is also moving with a positive velocity. However, because it is slowing down while moving with a positive velocity, its acceleration is considered negative. (This can be viewed in a mathematical manner as well. If the car was originally moving with a velocity of +25 m/s, it is finishing with a speed less than that, like +5 m/s. Because the change in velocity is negative, the acceleration will be as well.)

Because the positive direction is considered to the right of the paper, Car C is moving with a positive velocity. Because all arrows are of the same length, this car is not changing its speed. As a result, its change in velocity is zero, and its acceleration must be zero as well.

Because the car is moving opposite to the positive direction, Car D is moving with a negative velocity. Because it is speeding up while moving in a negative direction, its acceleration is negative as well.

Because it is moving opposite to the positive direction, Car E is moving with a negative velocity as well. However, because it is slowing down while moving in a negative direction, its acceleration is actually positive. As in example B, this may be more easily understood in a mathematical sense. The car is originally moving with a large negative velocity (−25 m/s) but slows to a final velocity that is less negative (−5 m/s). This change in velocity, from −25 m/s to −5 m/s, is actually a positive change ( ${v}_{f}-{v}_{i}=-5\text{m/s}--25\text{m/s}$ of 20 m/s. Because the change in velocity is positive, the acceleration must also be positive.

### Making Connection - Illustrative Example

The three graphs below are labeled A, B, and C. Each one represents the position of a moving object plotted against time.

As we did in the previous example, let's consider the acceleration and velocity of each object in terms of its direction of travel.

Object A is continually increasing its position in the positive direction. As a result, its velocity is considered positive.

During the first portion of time (shaded grey) the position of the object does not change much, resulting in a small positive velocity. During a later portion of time (shaded green) the position of the object changes more, resulting in a larger positive velocity. Because this positive velocity is increasing over time, the acceleration of the object is considered positive.

As in case A, Object B is continually increasing its position in the positive direction. As a result, its velocity is considered positive.

During the first portion of time (shaded grey) the position of the object changes a large amount, resulting in a large positive velocity. During a later portion of time (shaded green) the position of the object does not change as much, resulting in a smaller positive velocity. Because this positive velocity is decreasing over time, the acceleration of the object is considered negative.

Object C is continually decreasing its position in the positive direction. As a result, its velocity is considered negative.

During the first portion of time (shaded grey) the position of the object does not change a large amount, resulting in a small negative velocity. During a later portion of time (shaded green) the position of the object changes a much larger amount, resulting in a larger negative velocity. Because the velocity of the object is becoming more negative during the time period, the change in velocity is negative. As a result, the object experiences a negative acceleration.

### Example 2.1

#### Calculating Acceleration: A Racehorse Leaves the Gate

A racehorse coming out of the gate accelerates from rest to a velocity of 15.0 m/s due west in 1.80 s. What is its average acceleration?

#### Strategy

First we draw a sketch and assign a coordinate system to the problem. This is a simple problem, but it always helps to visualize it. Notice that we assign east as positive and west as negative. Thus, in this case, we have negative velocity.

We can solve this problem by identifying $\mathrm{\Delta}v$ and $\mathrm{\Delta}t$ from the given information and then calculating the average acceleration directly from the equation $\stackrel{-}{a}=\frac{\mathrm{\Delta}v}{\mathrm{\Delta}t}=\frac{{v}_{\mathrm{f}}-{v}_{0}}{{t}_{\mathrm{f}}-{t}_{0}}$.

#### Solution

1. Identify the knowns. ${v}_{0}=0$, ${v}_{\mathrm{f}}=-\text{15}\text{.0 m/s}$ (the minus sign indicates direction toward the west), $\mathrm{\Delta}t=1\text{.80 s}$.

2. Find the change in velocity. Since the horse is going from zero to $-\text{15.0 m/s}$, its change in velocity equals its final velocity: $\mathrm{\Delta}v={v}_{\mathrm{f}}=-\text{15}\text{.0 m/s}$.

3. Plug in the known values ($\mathrm{\Delta}v$ and $\mathrm{\Delta}t$) and solve for the unknown $\stackrel{-}{a}$.

#### Discussion

The minus sign for acceleration indicates that acceleration is toward the west. An acceleration of $8\text{.33 m}{\text{/s}}^{2}$ due west means that the horse increases its velocity by 8.33 m/s due west each second, that is, 8.33 meters per second per second, which we write as $8\text{.33 m}{\text{/s}}^{2}$. This is truly an average acceleration, because the ride is not smooth. We shall see later that an acceleration of this magnitude would require the rider to hang on with a force nearly equal to his weight.

### Instantaneous Acceleration

Instantaneous acceleration $a$, or the *acceleration at a specific instant in time*, is obtained by the same process as discussed for instantaneous velocity in Time, Velocity, and Speed—that is, by considering an infinitesimally small interval of time. How do we find instantaneous acceleration using only algebra? The answer is that we choose an average acceleration that is representative of the motion. Figure 2.29 shows graphs of instantaneous acceleration versus time for two very different motions. In Figure 2.29(a), the acceleration varies slightly and the average over the entire interval is nearly the same as the instantaneous acceleration at any time. In this case, we should treat this motion as if it had a constant acceleration equal to the average (in this case about $1\text{.}\mathrm{8\; m}{\text{/s}}^{2}$). In Figure 2.29(b), the acceleration varies drastically over time. In such situations it is best to consider smaller time intervals and choose an average acceleration for each. For example, we could consider motion over the time intervals from 0 to 1.0 s and from 1.0 to 3.0 s as separate motions with accelerations of $+3\text{.}\mathrm{0\; m}{\text{/s}}^{2}$ and $\text{\u20132}\text{.}\mathrm{0\; m}{\text{/s}}^{2}$, respectively.

The next several examples consider the motion of the subway train shown in Figure 2.30. In (a) the shuttle moves to the right, and in (b) it moves to the left. The examples are designed to further illustrate aspects of motion and to illustrate some of the reasoning that goes into solving problems.

### Example 2.2

#### Calculating Displacement: A Subway Train

What are the magnitude and sign of displacements for the motions of the subway train shown in parts (a) and (b) of Figure 2.30?

#### Strategy

A drawing with a coordinate system is already provided, so we don't need to make a sketch, but we should analyze it to make sure we understand what it is showing. Pay particular attention to the coordinate system. To find displacement, we use the equation $\mathrm{\Delta}x={x}_{\mathrm{f}}-{x}_{0}$. This is straightforward since the initial and final positions are given.

#### Solution

1. Identify the knowns. In the figure we see that ${x}_{\mathrm{f}}=\text{6.70 km}$ and ${x}_{0}=\text{4.70 km}$ for part (a), and ${x\prime}_{\mathrm{f}}=3\text{.75 km}$ and ${x\prime}_{0}=5\text{.25 km}$ for part (b).

2. Solve for displacement in part (a).

3. Solve for displacement in part (b).

#### Discussion

The direction of the motion in (a) is to the right and therefore its displacement has a positive sign, whereas motion in (b) is to the left and thus has a minus sign.

### Example 2.3

#### Comparing Distance Traveled with Displacement: A Subway Train

What are the distances traveled for the motions shown in parts (a) and (b) of the subway train in Figure 2.30?

#### Strategy

To answer this question, think about the definitions of distance and distance traveled, and how they are related to displacement. Distance between two positions is defined to be the magnitude of displacement, which was found in Example 2.2. Distance traveled is the total length of the path traveled between the two positions. (See Displacement.) In the case of the subway train shown in Figure 2.30, the distance traveled is the same as the distance between the initial and final positions of the train.

#### Solution

1. The displacement for part (a) was +2.00 km. Therefore, the distance between the initial and final positions was 2.00 km, and the distance traveled was 2.00 km.

2. The displacement for part (b) was $\text{\u22121.5 km.}$ Therefore, the distance between the initial and final positions was 1.50 km, and the distance traveled was 1.50 km.

#### Discussion

Distance is a scalar. It has magnitude but no sign to indicate direction.

### Example 2.4

#### Calculating Acceleration: A Subway Train Speeding Up

Suppose the train in Figure 2.30(a) accelerates from rest to 30.0 km/h in the first 20.0 s of its motion. What is its average acceleration during that time interval?

#### Strategy

It is worth it at this point to make a simple sketch:

This problem involves three steps. First we must determine the change in velocity, then we must determine the change in time, and finally we use these values to calculate the acceleration.

#### Solution

1. Identify the knowns. ${v}_{0}=0$ (the trains starts at rest), ${v}_{\mathrm{f}}=\text{30}\text{.}\text{0 km/h}$, and $\mathrm{\Delta}t=\text{20}\text{.}\text{0 s}$.

2. Calculate $\mathrm{\Delta}v$. Since the train starts from rest, its change in velocity is $\mathrm{\Delta}v\text{=}\phantom{\rule{0.20em}{0ex}}\text{+}\text{30.0 km/h}$, where the plus sign means velocity to the right.

3. Plug in known values and solve for the unknown, $\stackrel{-}{a}$.

4. Since the units are mixed (we have both hours and seconds for time), we need to convert everything into SI units of meters and seconds. (See Physical Quantities and Units for more guidance.)

#### Discussion

The plus sign means that acceleration is to the right. This is reasonable because the train starts from rest and ends up with a velocity to the right (also positive). So acceleration is in the same direction as the *change* in velocity, as is always the case.

### Example 2.5

#### Calculate Acceleration: A Subway Train Slowing Down

Now suppose that at the end of its trip, the train in Figure 2.30(a) slows to a stop from a speed of 30.0 km/h in 8.00 s. What is its average acceleration while stopping?

#### Strategy

In this case, the train is decelerating and its acceleration is negative because it is toward the left. As in the previous example, we must find the change in velocity and the change in time and then solve for acceleration.

#### Solution

1. Identify the knowns. ${v}_{0}=\text{30}\text{.0 km/h}$, ${v}_{\mathrm{f}}=\mathrm{0\; km/h}$ (the train is stopped, so its velocity is 0), and $\mathrm{\Delta}t=\text{8.00 s}$.

2. Solve for the change in velocity, $\mathrm{\Delta}v$.

3. Plug in the knowns, $\mathrm{\Delta}v$ and $\mathrm{\Delta}t$, and solve for $\stackrel{-}{a}$.

4. Convert the units to meters and seconds.

#### Discussion

The minus sign indicates that acceleration is to the left. This sign is reasonable because the train initially has a positive velocity in this problem, and a negative acceleration would oppose the motion. Again, acceleration is in the same direction as the *change* in velocity, which is negative here. This acceleration can be called a deceleration because it has a direction opposite to the velocity.

The graphs of position, velocity, and acceleration vs. time for the trains in Example 2.4 and Example 2.5 are displayed in Figure 2.33. (We have taken the velocity to remain constant from 20 to 40 s, after which the train decelerates.)

### Example 2.6

#### Calculating Average Velocity: The Subway Train

What is the average velocity of the train in part b of Example 2.2, and shown again below, if it takes 5.00 min to make its trip?

#### Strategy

Average velocity is displacement divided by time. It will be negative here, since the train moves to the left and has a negative displacement.

#### Solution

1. Identify the knowns. ${x\prime}_{\mathrm{f}}=3\text{.75 km}$, ${x\prime}_{0}=\text{5.25 km}$, $\mathrm{\Delta}t=\text{5.00 min}$.

2. Determine displacement, $\mathrm{\Delta}x\prime $. We found $\mathrm{\Delta}x\prime $ to be $-\text{1.5 km}$ in Example 2.2.

3. Solve for average velocity.

4. Convert units.

#### Discussion

The negative velocity indicates motion to the left.

### Example 2.7

#### Calculating Deceleration: The Subway Train

Finally, suppose the train in Figure 2.34 slows to a stop from a velocity of 20.0 km/h in 10.0 s. What is its average acceleration?

#### Strategy

Once again, let's draw a sketch:

As before, we must find the change in velocity and the change in time to calculate average acceleration.

#### Solution

1. Identify the knowns. ${v}_{0}=-\text{20 km/h}$, ${v}_{\mathrm{f}}=\mathrm{0\; km/h}$, $\mathrm{\Delta}t=\text{10}\text{.}\mathrm{0\; s}$.

2. Calculate $\mathrm{\Delta}v$. The change in velocity here is actually positive, since

3. Solve for $\stackrel{-}{a}$.

4. Convert units.

#### Discussion

The plus sign means that acceleration is to the right. This is reasonable because the train initially has a negative velocity (to the left) in this problem and a positive acceleration opposes the motion (and so it is to the right). Again, acceleration is in the same direction as the *change* in velocity, which is positive here. As in Example 2.5, this acceleration can be called a deceleration since it is in the direction opposite to the velocity.

### Sign and Direction

Perhaps the most important thing to note about these examples is the signs of the answers. In our chosen coordinate system, plus means the quantity is to the right and minus means it is to the left. This is easy to imagine for displacement and velocity. But it is a little less obvious for acceleration. Most people interpret negative acceleration as the slowing of an object. This was not the case in Example 2.7, where a positive acceleration slowed a negative velocity. The crucial distinction was that the acceleration was in the opposite direction from the velocity. In fact, a negative acceleration will *increase* a negative velocity. For example, the train moving to the left in Figure 2.34 is sped up by an acceleration to the left. In that case, both $v$ and $a$ are negative. The plus and minus signs give the directions of the accelerations. If acceleration has the same sign as the velocity, the object is speeding up. If acceleration has the opposite sign as the velocity, the object is slowing down.

### Check Your Understanding

An airplane lands on a runway traveling east. Describe its acceleration.

Learn about position, velocity, and acceleration graphs. Move the little man back and forth with the mouse and plot his motion. Set the position, velocity, or acceleration and let the simulation move the man for you.