Unit2_VirtualLabImpulse_Momentum (1)
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School
Lansing Community College *
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Course
221
Subject
Electrical Engineering
Date
Apr 3, 2024
Type
Pages
7
Uploaded by ChefDiscoveryEmu25
Experiment
20
Virtual Lab: Impulse and Momentum
*Please Note* If you will be submitting your assignment electronically please use a different
color of text for your answers. Thank you.
The impulse-momentum theorem relates impulse, the average force applied to an object times the
length of time the force is applied, and the change in momentum of the object:
Here we will only consider motion and forces along a single line. The average force,
F ,
is the
net
force on the object, but in the case where one force dominates all others it is sufficient to use only
the large force in calculations and analysis.
For this experiment, a dynamics cart connected to an elastic tether will roll along a level track.
Momentum is conserved if there is not net external force acting on the system. If we consider the
system frictionless momentum is conserved until the elastic tether becomes taunt. Its momentum
will change as it reaches the end of an initially slack elastic tether cord, much like a horizontal
bungee jump. The tether will stretch and apply an increasing force until the cart stops. The cart
then changes direction and the tether will soon go slack. The force applied by the cord is measured
by a Force Sensor. The time starts when the force is first felt and continues until the tether goes
slack again. The cart velocity throughout the motion is measured with a Motion Detector. Using
Logger
Pro
to find the average force during a time interval, you can test the impulse-momentum
theorem.
Physics with Computers
20 - 1
Experiment 20
Objectives
●
Measure a cart’s momentum change and compare to the impulse it receives.
●
Compare average and peak forces in impulses.
Materials
Computer
dynamics cart and track
Vernier computer interface
clamp
Logger
Pro
elastic cord
Vernier Motion Detector
Vernier Force Sensor
string
500 g mass
bubble level
Preliminary questions and discussion
Please take some time to answer the questions below.
1.
In a car collision, the driver’s body must change speed from a high value to zero. This is true
whether or not an airbag is used, so why use an airbag? How does it reduce injuries?
When a car crash happens the people inside are moving at a fast speed and suddenly they need to
stop. This sudden stop could cause serious injuries because their bodies feel a big force. Airbags
are a cushion for you to hit which makes the stop happen more slowly spreading the force and
helps prevent injuries, especially to your head. even though you still stop suddenly the airbag
helps reduce injuries.
2.
You want to close an open door by throwing either a 400 g lump of clay or a 400 g rubber ball
toward it. You can throw either object with the same speed, but they are different in that the
rubber ball bounces off the door while the clay just sticks to the door. Which projectile will
apply the larger impulse to the door and be more likely to close it?
When you throw both a rubber ball and a lump of clay with the same force the rubber ball hits
the door and bounces back, pushing the door harder, but the clay just sticks to the door so it
doesn’t push as much. Because the rubber ball gives a stronger push or impulse to the door the
bouncing back, is like hitting it twice and is more likely to close the door compared to the lump
of clay.
20 - 2
Physics with Computers
Impulse and Momentum
3.
View the following video discussing these questions and the lab experiment:
Impulse & Momentum Pre-Lab Video https://youtu.be/yVJyIZ65vzE
Procedure
The following procedure will be conducted by an instructor in lab as your “virtual lab partner”
please be sure to record the data that is obtained during the experiment in the video in the
following data table because you will be conducting the data analysis on your own. Please follow
along with the experiment in this video:
Impulse & Momentum Lab Experiment
https://youtu.be/DBi2gc9BmNI
1.
Measure the mass of your dynamics cart plus any weights placed on the cart and record the
value in the data table.
2.
Connect the Motion Detector to DIG/SONIC 1 of the interface. Connect the Force Sensor to
Channel 1 of the interface. If your Force Sensor has a range switch, set it to 10 N.
3.
Open the file “20 Impulse and Momentum” in the
Physics with Vernier
folder. Logger Pro
will
plot the cart’s position and velocity
vs
. time, as well as the force applied by the Force Sensor
vs
.
time.
4.
Calibrate the Force Sensor.
a. Choose Calibrate
±
CH1: Dual Range Force from the Experiment menu. (Click on the
Calibrate Tab if it is not already the open tab.) Click
.
b. Remove all force from the Force Sensor. Enter a
0
(zero) in the Reading 1 field. Hold the
sensor vertically with the hook downward and wait for the reading shown for CH1 to
stabilize. Click
. This defines the zero force condition.
c.
Hang the 500 g mass from the sensor. This applies a force of 4.905 N. Enter
4.905
in the
Reading 2 field, and after the reading shown for CH1 is stable (If the weight is swinging it will
take longer to stabilize, also the number may continue to change between 2 digits in the last
decimal place.), click
. Click
to close the calibration dialog.
5.
Place the track on a level surface. Confirm that the track is level by placing the bubble level on
it. Also check by placing the low-friction cart on the track and releasing it from rest since the
track can be warped in one spot.. It should not roll. If necessary, adjust the track.
6.
Attach the elastic cord to the cart and then the cord to the string. Tie the string to the Force
Sensor a short distance away. Choose a string length so that the cart can roll freely with the
cord slack for most of the track length, but be stopped by the cord before it reaches the end of
the track. Clamp the Force Sensor so that the string and cord, when taut, are horizontal and in
line with the cart’s motion.
Physics with Computers
20 - 3
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Experiment 20
7.
Place the Motion Detector (on the cart reading) beyond the other end of the track so that the
detector has a clear view of the cart’s motion along the entire track length. When the cord is
stretched to maximum extension the cart should not be closer than 0.2 m to the detector.
8.
Click
, select Force Sensor from the list, and click
to zero the Force Sensor.
9.
Practice releasing the cart so it rolls toward the Motion Detector, bounces gently, and returns
to your hand. The Force Sensor must not shift and the cart must stay on the track. Arrange the
cord and string so that when they are slack they do not interfere with the cart motion. You may
need to guide the string by hand, but be sure that you do not apply any force to the cart or
Force Sensor. Keep your hands away from between the cart and the Motion Detector.
10.
Click
to take data; roll the cart and confirm that the Motion Detector detects the cart
throughout its travel. Inspect the force data. If the peak exceeds 10 N, then the applied force is
too large. Roll the cart with a lower initial speed. If the velocity graph has a flat area when it
crosses the time-axis, the Motion Detector was too close and the run should be repeated.
11.
Once you have made a run with good position, velocity, and force graphs, analyze your data. To
test the impulse-momentum theorem, you need the velocity before and after the impulse.
Choose an interval corresponding to a time when the elastic was initially relaxed, and the cart
was moving at approximately constant speed away from the Force Sensor. Drag the mouse
pointer across this interval. Click the Statistics button,
, and read the average velocity.
Record the value for the initial velocity in your data table. In the same manner, choose an
interval corresponding to a time when the elastic was again relaxed, and the cart was moving
at approximately constant speed toward the Force Sensor. Drag the mouse pointer across this
interval. Click the statistics button and read the average velocity. Record the value for the final
velocity in your data table.
12.
Now record the time interval of the impulse. On the force
vs.
time graph, drag across the
impulse, capturing the entire period when the force was non-zero. Find the average value of
the force by clicking the Statistics button,
, and also read the length of the time interval over
which your average force is calculated. This can be found at the bottom of the force graph as
the
x.
13.
Perform a 3 more trials by repeating Steps 10 – 12. Try to make the force a little different each
time. Record the information in your data table.
20 - 4
Physics with Computers
Impulse and Momentum
Data Table
The mass of the cart was measured to be 490.6 grams which is converted to 0.4906 kilograms.
Mass of cart + weights
0.4906 kg
Trial
Final
Velocity
vf
(m/s)
Initial
Velocity
vi
(m/s)
Average
Force
F
(N)
Duration
of
Impulse
Δ
t
(s)
1
1.027
-1.151
0.9394
1.148
2
0.7280
-0.8525
0.7501
1.061
3
0.8380
-0.9902
0.5915
1.077
4
0.8677
-1.001
0.6030
1.074
5
0.7733
-0.8980
0.8082
1.036
Physics with Computers
20 - 5
Experiment 20
Analysis
1.
From the mass of the cart and change in velocity, determine the final and initial momentum
and the change in momentum as a result of the impulse. Make this calculation for each trial
and enter the values in the second data table found at the end of this section.
2.
Determine the impulse for each trial from the average force and time interval values. Record
these values in your data table.
3.
If the impulse-momentum theorem is correct, the change in momentum will equal the impulse
for each trial. Experimental measurement errors, along with friction and shifting of the track or
Force Sensor, will keep the two from being exactly the same. One way to compare the two is to
find their percentage difference. Divide the difference between the two values by the average
of the two, then multiply by 100%. How close are your values, percentage-wise? Do your data
support the impulse-momentum theorem?
We calculated the percentage difference between the change in momentum and impulse to see
how closely they match. The percentage difference is small in trial 1 and trial 5, this means the
change in momentum and impulse are close supporting the theorem. But in trials 2,3 and 4 there
was a big difference between the change in momentum and impulse, around a 30 to 35%
difference. This shows that the data might not fully support the term possibly due to
measurement error, and other factors.
4.
Look at the shape of the force
vs
. time graph of your last trial. Is the peak value of the force
significantly different from the average force? Is there a way you could deliver the same
impulse with a much smaller force?
The peak value of the force is different from the average force. This means the force applied
during impact is not consistent. It starts strong and then gets weaker. To deliver the same
impulse with a smaller force we can make the collision last longer by spreading the force over
time. This will reduce the peak force while still giving the same push.
5.
Revisit your answers to the Preliminary Questions in light of your work with the
impulse-momentum theorem.
After you have completed your calculations in the table as well as answered all of the prelab and
analysis questions (in a different color of text) be sure to submit your handout to your instructor.
Calculations Table
20 - 6
Physics with Computers
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Impulse and Momentum
Trial
Final
Momentum
m vf
Initial
Momentum
m vi
Change in
momentum
Δ
mom
Impulse
F
Δ
t
Average of
change in
momentum &
Impulse
(
Δ
mom
+
F
Δ
t)/2
Difference
between change
in momentum &
Impulse
|(
Δ
mom
-
F
Δ
t)|
% difference between
Impulse and Change
in momentum
|(
Δ
mom
-
F
Δ
t)| *
100
Average
units
(kg
⋅
m/s)
(kg
⋅
m/s)
(kg
⋅
m/s)
or (N
⋅
s)
(N
⋅
s)
(N
⋅
s)
(N
⋅
s)
%
1
0.504
-0.564
1.068
1.078
1.073
0.01
0.93%
2
0.357
-0.418
0.775
0.796
0.786
0.21
26.72%
3
0.411
-0.486
0.897
0.637
0.767
0.26
33.90%
4
0.427
-0.491
0.918
0.648
0.783
0.27
34.48%
5
0.379
-0.441
0.82
0.837
0.829
0.017
2.05%
After you have completed your calculations in the table as well as answered all of the prelab and
analysis questions (in a different color of text) be sure to submit your handout to your instructor.
Physics with Computers
20 - 7
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