As you read, pay attention to the relevant equations in the box Kinematics Equations for Objects in Free Fall where Acceleration = −g
Note that because the motion is free fall, a is simply replaced with (here,
is the acceleration due to gravity,
) and the direction of motion is the
direction, rather than the
direction. When calculating the position and velocity of an object in freefall, we need to consider two different conditions. First, the object can be thrown up as it enters freefall. For example, you could throw a baseball up and watch it fall back down.
Complete the steps in Example 2.14. After you review the solution, pay attention to the graphs in Figure 2.40. You can throw an object directly downward as it enters freefall, such as when you throw a baseball directly down from a second-floor window.
Then, complete the steps in Example 2.15. Notice that Figure 2.42 compares what is happening in Example 2.14 and Example 2.15. It is important to understand the difference between an object that is thrown up and enters free fall, versus an object that is directly thrown down. We can often use experimental data to calculate constants, such as .
In Example 2.16, we determine the acceleration due to gravity constant () from experimental data.
Example 2.16 Find \(\boldsymbol{g}\) from Data on a Falling Object
Example 2.16 Find
from Data on a Falling Object
The acceleration due to gravity on Earth differs slightly from place to place, depending on topography (e.g., whether you are on a hill or in a valley) and subsurface geology (whether there is dense rock like iron ore as opposed to light rock like salt beneath you). The precise acceleration due to gravity can be calculated from data taken in an introductory physics laboratory course.
An object, usually a metal ball for which air resistance is negligible, is dropped and the time it takes to fall a known distance is measured. See, for example, Figure 2.43. Very precise results can be produced with this method if sufficient care is taken in measuring the distance fallen and the elapsed time.
Figure 2.43 Positions and velocities of a metal ball released from rest when air resistance is negligible. Velocity is seen to increase linearly with time while displacement increases with time squared. Acceleration is a constant and is equal to gravitational acceleration.
Suppose the ball falls 1.0000 m in 0.45173 s. Assuming the ball is not affected by air resistance, what is the precise acceleration due to gravity at this location?
Strategy
Draw a sketch.
Figure 2.44
We need to solve for acceleration . Note that in this case, displacement is downward and therefore negative, as is acceleration.
Solution
2. Choose the equation that allows you to solve for using the known values.
3. Substitute 0 for and rearrange the equation to solve for
. Substituting 0 for
yields
4. Substitute known values yields
so, because with the directions we have chosen,
Discussion
The negative value for indicates that the gravitational acceleration is downward, as expected. We expect the value to be somewhere around the average value of
, so
makes sense. Since the data going into the calculation are relatively precise, this value for
is more precise than the average value of
; it represents the local value for the acceleration due to gravity.