11.) Lab 127_ Torque & Rotational Inertia
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Mechanical Engineering
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Feb 20, 2024
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Lab
127:
Torque
&
Rotational
Inertia
A.
Introduction:
Theory
&
Objectives
Similar to how angular acceleration is accretion in a circular motion, torque is the
force applied to make an object move in a circular motion. As the relation indicates, the
force times the radius equals torque. However, like force, torque does not equal ma, it
instead equals the angular accretion times a different time of inertia, rotational inertia. This
hybrid equation is given below:
Στ = 𝐼α
Like normal inertia is in a sense the resistance that is felt when accelerating an object,
rotational inertia is the resistance felt when angularly accelerating an object. Differently
again, the rotational inertia is not just the mass but a compilation of other factors present
when in a circular motion. The equations for rotational inertia are below:
𝐼 = Σ𝑚
𝑖
𝑟
𝑖
2
With these two given distinctions from normal linear motion, all the other laws of
physics can be applied. To understand the further workings of these elements of circular
motion, in this lab, we will explore how the force of tension and force of gravity impact the
movement of disks and rings. Compostitly, we will also observe and estimate how that
motion changes when the same forces are applied at different locations and at different
angles.
B.
Experimental
Procedure
1.
With the given values, theoretically calculate the rotational inertia of a disk (center and
diameter) and a ring.
2.
Measure the diameter of the pulley for further calculations, and place the disk in the
shaft, stimulating Figure 4.
3.
Place the 50g hangers on the disks, and 200g weight on the pulley.
4.
Click record and release the thread, observe the speed vs. time graph, and derive for
linear accretion. Repeat two more times and average for a more accurate result.
5.
Set up the pulley and disk according to Figure 5 and place the ring into the groove on
the disk.
6.
Then, once again let go of the strong while recording, and then find the acceleration
by deriving the speed vs. time graph.
7.
When doing the rotational inertia for the ring alone, the rotational inertia of the disk
must be subtracted.
8.
Now, one last time takes everything apart and simulates the diagram in Figure 6. Next,
let the strong loose and record.
9.
Find the accretion with the slope of the speed vs. time graph, and then the rotational
inertia by subtracting away some of the previously found properties.
C.
Results:
Data
&
Calculations
Qualities:
Disk
Ring
Mass
1.4035
1.4264
Radius
.115
.0525
.0625
Rotational
Inertia
Center of Mass: .00927
.00475
Diameter: .00464
Case
Run
Linear (a)
Tension
Torque
Angular (
α
)
Total (
I
)
Disk
1
0.0414
2.44
0.0305
3.31
.009208
2
0.0415
2.44
0.0305
3.32
.009185
3
0.0414
2.44
0.0305
3.31
.009208
Step-Pulle
y & Shaft
1
7.37
0.61
0.00759
589.6
.000013
2
7.39
0.60
0.00753
591.2
.000013
3
7.35
0.61
0.00766
588
.000013
Disk &
Ring
1
0.0278
2.44
0.0305
2.22
.013731
2
0.027
2.44
0.0305
2.16
.014139
3
0.0271
2.44
0.0305
2.17
.014087
Disk
2
1
0.0755
2.43
0.0304
6.04
.005031
2
0.0755
2.431125
0.0304
6.04
.005031
3
0.0767
2.430825
0.0304
6.14
.004952
Case
Theoretical
I
Experimental
I
%
Error
Disk
1
.00927
.0092003
.752 %
Disk
2
.00464
.00500
7.2 %
Disk
+
Ring
.00475
.004716
.7209 %
In this lab, we are theoretically and experimentally finding the rotational inertia of
various objects. We started off by measuring the rotational inertia of just the disk by
measuring its linear speed. By obtaining the linear speed we were able to find the linear
acceleration via calculus. Then, with the given accelerations we were able to find the
magnitude of the other forces involved in the experiment with Newton’s Laws. Furthermore,
with the linear acceleration, we were also able to find the angular acceleration due to their
radial relationship. Lastly, with the secondary results of the angular acceleration, we were
able to find the Rotational Inertia. We repeated this process of calculations with various
setups to see and understand how different weights and weight distribution dynamics
change the accelerations and inertia To add, we were in a way able to estimate the
rotational inertia of certain components in a system where we knew the total inertia and
other components’ inertia as well. This additive property of inertia has allowed us to find the
inertia of almost every single in the setup.
D.
Discussion:
Error
Analysis/Questions
1.) How good is your experiment result compared to the theoretical one? What could be
the possible error of sources?
On the large scale of things, both our experimental and theoretical values for all three
cases were very similar. In fact, our percent error for the Disk through the center of mass
and Ring is about .7%. Our error was so small that it could possibly be assumed as
negligible. However, for the disk through the diameter we had an error of 7.2%. This is
about 10 times the error we had for the other two. I think this error was actually caused by
us experimenters. I think we may have set the experiment somehow wrong, or weren't
entirely sure about the placement and angles of all the components of the setup. If given
another chance, perhaps we would be more vigilant about the setup for this case and make
sure that it is more accurate than the diagram given in the lab manual.
2.)
Error
Analysis
in
the
previous
question.
E.
Conclusion
of
Experiment
In this lab, I think I was able to use so many different concepts at the same time.
When actually doing the lab, I was kind of confused about the whole setup and the overall
purpose of the lab. But after completing it, it makes a lot of sense. I personally enjoyed
doing all the calculations because I was able to use old concepts like F = ma, and also use
recent topics like torque and angular acceleration. Combining all these ideologies and then
further calculating the rotational inertia was very intriguing to me. It made me actually think
through all the concepts, and understand the indirect relationships. I was able to solidify my
knowledge of angular motion a lot more in this lab.
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