Read this text. Pay attention to the examples which show how to solve equations of motion. These include how to calculate displacement, given average velocity and time, and how to calculate final velocity, given initial velocity, acceleration, and time.
Example 2.1 Calculating Acceleration: A Racehorse Leaves the Gate
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?
Figure 2.15
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.
Figure 2.16
We can solve this problem by identifying \(\Delta v\) and \(\Delta t\) from the given information and then calculating the average acceleration directly from the equation \(\bar{a}=\frac{\Delta v}{\Delta t}=\frac{v_{\mathrm{f}}-v_{0}}{t_{\mathrm{f}}-t_{0}}\).
Solution
1. Identify the knowns. \(v_{0}=0, v_{\mathrm{f}}=-15.0 \mathrm{~m} / \mathrm{s}\) (the negative sign indicates direction toward the west), \(\Delta t=1.80 \mathrm{~s}\)
2. Find the change in velocity. Since the horse is going from zero to \(-15.0 \mathrm{~m} / \mathrm{s}\), its change in velocity equals its final velocity: \(\Delta v=v_{\mathrm{f}}=-15.0 \mathrm{~m} / \mathrm{s}\).
3. Plug in the known values \((\Delta v\) and \(\Delta t)\) and solve for the unknown \(\bar{a}\).
\(\bar{a}=\frac{\Delta v}{\Delta t}=\frac{-15.0 \mathrm{~m} / \mathrm{s}}{1.80 \mathrm{~s}}=-8.33 \mathrm{~m} / \mathrm{s}^{2}.\)
Discussion
The negative sign for acceleration indicates that acceleration is toward the west. An acceleration of \(8.33 \mathrm{~m} / \mathrm{s}^{2}\) due west means that the horse increases its velocity by \(8.33 \mathrm{~m} / \mathrm{s}\) due west each second, that is, \(8.33\) meters per second per second, which we write as \(8.33 \mathrm{~m} / \mathrm{s}^{2}\). 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.