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Calculate the acceleration of gravity using simple materials, a cell phone, and a computer to record, watch, and analyze the motion of a dropped object.
Collect your data
Have one partner stand next to the measuring tape. Turn on the flashlight and point it upwards. Make sure your flashlight is on a non-blinking setting. Place the light as close to the 0 cm mark as possible and against the measuring tape. If possible, use only one finger to hold the flashlight still until the time of release. Have someone else film the drop with a digital camera (in HD at standard 30 frames per second).
Check your video to make sure you got the shot. Digital video is easy to erase and reshoot. Redo it if you didn’t get a clear view of your flashlight’s light falling straight down. Transfer your video file to a computer.
Record your data
Make a table with two columns to record your data. Label the columns “Time in seconds” and “Distance in meters.” (See the sample table below.)
Time Data: Since your camera records 30 frames a second, each frame represents only 1/30 of a second, or about 0.033 seconds. That means each frame will add an additional 0.033 seconds.
Distance Data: In your video player, find the frame just before your flashlight drops. (Note that frame-by-frame players usually let you move forward or backward via arrow keys. The frame you’re now at is time 0s and distance 0m.)
Now, step by step, record the distance in meters dropped and the corresponding time of the flashlight’s fall. Watch the screen closely. Notice that, during the first few steps, the flashlight doesn’t fall very much.
If your flashlight leaves a streak of light, only record the location at the bottom of the streak (the streak is a 1/30th of a second record of the light's fall).
Calculate the acceleration due to gravity
Acceleration describes how fast the rate of something changes.
Acceleration = (Vfinal – Vinitial) / the time to make this change
Here’s an example using our data (see the table above):
Vinitial is the flashlight’s velocity just before it’s dropped, or 0 m/s; Vfinal is the velocity of the light at the end of the drop.
In our case, at time 0.297 to 0.33 s (time = 0.033 s), the distance traveled is from 0.4 m to 0.51 m (distance = 0.11 m).
V = distance / time
So, Vfinal = 0.11 m / 0.033 s = 3.33 m/s
The time it takes to make that change is 0.33 s
Acceleration = (3.33 m/s – 0 m/s) / 0.33 s = 10 m/s2
Use your own data to calculate the acceleration of the flashlight you drop.
In your own experiments, you can collect data from shorter or longer distances.
Gravity is a force that draws objects to one another. In this case, the objects are the flashlight and the earth. This fundamental interaction of nature causes objects like the flashlight to move toward the earth faster and faster.
Look at your data. You might notice that the distances between successive time intervals increases. This also means the object’s velocity is increasing, and increasing velocity is known as acceleration. You might have heard a car commercial use the phrase “Zero to sixty in five seconds,” or some such thing. That means the car went from one velocity to another in a certain period of time—that’s acceleration!
Things accelerate toward the earth at a constant rate. Your data should show that this rate is about 9.8 meters per second per second, or 9.8 m/s2. Scientists, engineers, teachers, and students also know this constant as, simply, g.
Graphing is a great way to see what’s going on with your data. Try plotting distance vs. time.
Is your graph a straight line? Is it a curve?
It should be a curve with the formula: d = 1/2 g t2. The graph of our sample data is shown below.
Put an object on a scale. Is it moving? Although it doesn’t look like it, your object is actually accelerating towards the earth. The scale’s pan is pushing again your object and forcing it from moving downward. The weight you read on your device is a result of the object’s mass and g.
Try doing this activity again, but drop lightweight objects with lots of surface area, such as coffee filters or feathers, and see how the results differ. Although g is still at work here, air resistance also plays a role.
See this Snack in action in this video.
Prove to yourself that Galileo was right.
Listen to the rhythm of falling weights.
Components of force make a toy walk and stop at just the right time.
This work is licensed under a Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International License.
Attribution: Exploratorium Teacher Institute