Lab finding the mass of a flywheel

In summary, the problem involves estimating the mass of a disc with a string attached to a hanging mass. The disc is wound up and the time it takes for the mass to fall to the ground is recorded. The equations used to solve for the mass include E_pot=E_k+E_rot, where E_pot is gravitational potential energy, E_k is kinetic energy, and E_rot is rotational kinetic energy. However, there may be a mistake in determining the final velocity due to the string being attached to an axle rather than wrapped around the disc. Additional information is needed, such as the radius of the axle and the length of the string.
  • #1
onelove8187
7
0

Homework Statement


The problem is I need to estimate the mass of a (solid equally distributed mass) disc which has an axle on which a string is tied and then attached to a (hanging) 1.022 kg mass. We wound the wheel up moving the hanging mass to a height of 0.64 m off the ground. At this point we recorded the time it would take for the mass to fall to the floor (spinning the wheel in the process). for this first run we have an average time t=10.42s. We did this several times varying the height off the floor of the hanging mass. We also ran several tests varying the mass. I have spent probably ten hours banging my head against a wall, I do not know what mistake I am making. This is what I tried to solve for the mass of the wheel in the first run:

E_pot=E_k+E_rot

E_pot=mgy
E_k(at bottom)=.5mv^2
E_rot=.5Iω^2 where I=.5MR^2 and ω=v/R

where m=known mass and M=mass of wheel

Combining all this I got:

mgy=.5mv^2+.5(.5MR^2)(v/R)^2

simplifying to

M=4m(gy-.5v^2)/v^2
for the first fun it gives≈1600kg as the answer which can't be right!

I also tried to solve this from a torque perspective and got the same answer!
possible other relevant equations:

angular acceleration=torque_net/Moment of Inertia
a_y=angular acceleration
Torque=Tension*d (where d=R in this case)

More than anything I want to see where my error in logic is here so I can better understand the material. Any help will be greatly appreciated. Thank you!
 
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  • #2
onelove8187 said:

Homework Statement


The problem is I need to estimate the mass of a (solid equally distributed mass) disc which has an axle on which a string is tied and then attached to a (hanging) 1.022 kg mass. We wound the wheel up moving the hanging mass to a height of 0.64 m off the ground. At this point we recorded the time it would take for the mass to fall to the floor (spinning the wheel in the process). for this first run we have an average time t=10.42s. We did this several times varying the height off the floor of the hanging mass. We also ran several tests varying the mass. I have spent probably ten hours banging my head against a wall, I do not know what mistake I am making. This is what I tried to solve for the mass of the wheel in the first run:

E_pot=E_k+E_rot

E_pot=mgy
E_k(at bottom)=.5mv^2
E_rot=.5Iω^2 where I=.5MR^2 and ω=v/R

where m=known mass and M=mass of wheel

Combining all this I got:

mgy=.5mv^2+.5(.5MR^2)(v/R)^2

simplifying to

M=4m(gy-.5v^2)/v^2
for the first fun it gives≈1600kg as the answer which can't be right!

I also tried to solve this from a torque perspective and got the same answer!
possible other relevant equations:

angular acceleration=torque_net/Moment of Inertia
a_y=angular acceleration
Torque=Tension*d (where d=R in this case)

More than anything I want to see where my error in logic is here so I can better understand the material. Any help will be greatly appreciated. Thank you!
Hi onlove8187. Welcome again to Physics Forums.
By the way, how did things work out with the first problem you posted? I noticed you did not respond to any of the replies given to your post.​



For this problem you found the following expression for the mass of the disc.

M=4m(gy-.5v2)/v2

This may well be the correct result.

You didn't mention how you determined v. I assume that's some velocity. Exactly what is that velocity?
 
Last edited:
  • #3
Thanks very much for responding. I found the velocity using kinematics. We recorded the time it took the block to fall to the ground and then with the known height and an initial velocity of 0 I found the acceleration using v_f=v_i+a(Δt). After that I found the final velocity with (V_f)^2=(V_i)^2+2a_y(Δx). My thinking is that at this point the final Kinetic Energy + rotational Kinetic energy should have come completely from the gravitational potential energy that was present when the block was at height h.
 
  • #4
onelove8187 said:
Thanks very much for responding. I found the velocity using kinematics. We recorded the time it took the block to fall to the ground and then with the known height and an initial velocity of 0 I found the acceleration using v_f=v_i+a(Δt). After that I found the final velocity with (V_f)^2=(V_i)^2+2a_y(Δx). My thinking is that at this point the final Kinetic Energy + rotational Kinetic energy should have come completely from the gravitational potential energy that was present when the block was at height h.

What did you use for the acceleration ?

In the equation, vf = vi + a(Δt), which you used to find a, you don't know vf either, do you ?
 
  • #5
SammyS said:
What did you use for the acceleration ?

In the equation, vf = vi + a(Δt), which you used to find a, you don't know vf either, do you ?


You are absolutely correct. My mistake, I used y_f=y_i+v_i *t+.5a_yt^2 where y_f is 0 and v_i is 0. Then I used that acceleration to find final velocity. I've been thinking, will the string being attached to the an axle change the approach. I think that may be where my mistake is. I sort of modeled it as if the string were wrapped around the disk and not around an axle in the center.
 
  • #6
onelove8187 said:
You are absolutely correct. My mistake, I used y_f=y_i+v_i *t+.5a_yt^2 where y_f is 0 and v_i is 0. Then I used that acceleration to find final velocity. I've been thinking, will the string being attached to the an axle change the approach. I think that may be where my mistake is. I sort of modeled it as if the string were wrapped around the disk and not around an axle in the center.
This suggests some additional questions.

Was the string was wrapped around the axle, or was it wrapped around the disc? In the former case you need to know the radius of the axle. Also, the analysis is more involved if the string wraps over itself so many times so that the effective radius "seen" by the string decreases significantly as the string unwinds.

Is the string longer than the initial distance of the hanging mass from the floor?


By the way:

If you can assume constant acceleration, then the average velocity is given by vavg = (vf + vi)/2
 
  • #7
The string was wrapped around the axle and we do know the radius of the axle. Also, it didn't wrap over itself too much changing the radius felt by the string. Lastly, yes the string was longer than required to reach the floor.
 
  • #8
onelove8187 said:
The string was wrapped around the axle and we do know the radius of the axle. Also, it didn't wrap over itself too much changing the radius felt by the string. Lastly, yes the string was longer than required to reach the floor.

So there's some additional algebra to do.

If the radius of the axle is r, then that must replace R in at least one of your basic equations.

Show what you get now.
 
  • #9
Ok I replaced the R in (v/R) with r and plugging it in got 12.002 kg which is a very reasonable answer. I understand the need to account for small radius of the axle; however, I'm not sure I see the clear connection. Why would it not matter which R I replace with r?
 
  • #10
onelove8187 said:
Ok I replaced the R in (v/R) with r and plugging it in got 12.002 kg which is a very reasonable answer. I understand the need to account for small radius of the axle; however, I'm not sure I see the clear connection. Why would it not matter which R I replace with r?
It's still true that I = (1/2) M R2. Right?

Really, unless you show the complete set of modified equations, it's difficult to comment on your updated result. Also, difficult to answer your most recent question definitively.
 
  • #11
SammyS said:
It's still true that I = (1/2) M R2. Right?

Really, unless you show the complete set of modified equations, it's difficult to comment on your updated result. Also, difficult to answer your most recent question definitively.


Here is where I am at:

Still am attempting an energy approach so E_pot=E_k+E_rot

I still have the same acceleration I calculated from the falling mass being dropped to the floor where
t=10.42s
y_i=.64m

so: a_y=(2y_i)/t^2 gives a_y=-.0118m/s^2

and the the final velocity of the falling block (as well as V_t for rotating axle) is then
v_f=√(2*a_y*y_i) gives v_f=.1229

E_pot=mgy
E_k=.5mv^2

and E_rot=.5Iω^2
ω=(v/r_axle) and I=.5M(R_disk)^2

so E_rot=.5(.5MR_disk^2)(v/r_axle)^2

giving mgy=.5mv^2+.5(.5MR_disk^2)(v/r_axle)^2

solving for M gives (4mr^2(gy-(v^2)/2))/R^2V^2

the other required experimental data is
R_disk=.2282m
r_axle=.0192m
mass of falling block= 1.022kg

so M=(4*1.022*0.0192^2(9.8*.64-(0.1229^2/2)))/(0.2282*0.1229^2) gives M=12.00

This seems to give me a reasonable answer and it's the only way I could think to incorporate the differences in velocity. I have tried numerous times to approach this from a torque perspective but am struggling to wrap my mind around it. What is the best way to solve this with torque?
 
  • #12
onelove8187 said:
Here is where I am at:

Still am attempting an energy approach so E_pot=E_k+E_rot

I still have the same acceleration I calculated from the falling mass being dropped to the floor where
t=10.42s
y_i=.64m

so: a_y=(2y_i)/t^2 gives a_y=-.0118m/s^2

and the the final velocity of the falling block (as well as V_t for rotating axle) is then
v_f=√(2*a_y*y_i) gives v_f=.1229
It's helpful to have these details.

That method does give the correct final velocity.


Notice that putting these two equations together gives to following.
##\displaystyle
v_f=\sqrt{2\left(\frac{2y_i}{t^2} \right)y_i\ }=2\frac{y_i}{t}\ .##​

This is consistent with ##\displaystyle \ v_\text{avg}=\frac{v_i+v_f}{2}\,,\ ## since ##\displaystyle \ v_\text{avg}=\frac{y_i}{t}##

(Using this directly gives vf = 0.12284... m/s , which is close to your result .)
... the other required experimental data are
R_disk=.2282m
r_axle=.0192m
mass of falling block= 1.022kg

so M=(4*1.022*0.0192^2(9.8*.64-(0.1229^2/2)))/(0.2282*0.1229^2) gives M=12.00

This seems to give me a reasonable answer and it's the only way I could think to incorporate the differences in velocity. I have tried numerous times to approach this from a torque perspective but am struggling to wrap my mind around it. What is the best way to solve this with torque?
Doing it with torque should give the same result (of course). Use a free body diagram for the hanging mass.

In this approach you don't need velocities, but do need the acceleration. Your calculation of ay should be adequate here.
 

1. How do you determine the mass of a flywheel in the lab?

To determine the mass of a flywheel in the lab, you will need to use a balance or scale. First, weigh the flywheel alone on the balance and record the mass. Then, add additional weights to the flywheel until it is balanced and record the total mass. Finally, subtract the original mass of the flywheel to determine the mass of the added weights.

2. What tools are needed to measure the mass of a flywheel in the lab?

The main tool needed to measure the mass of a flywheel in the lab is a balance or scale. Additionally, you may need weights to add to the flywheel to balance it. A ruler or caliper may also be helpful for measuring the dimensions of the flywheel.

3. What are the units of measurement for the mass of a flywheel?

The mass of a flywheel is typically measured in grams (g) or kilograms (kg) in the lab. However, depending on the size and weight of the flywheel, other units of mass may be used such as milligrams (mg) or pounds (lbs).

4. Why is it important to accurately measure the mass of a flywheel in the lab?

Accurately measuring the mass of a flywheel is important because it is a crucial factor in determining its rotational inertia, or resistance to changes in its rotational motion. This information is important in various fields of science and engineering, such as in designing machines and understanding the laws of motion.

5. Are there any safety precautions to keep in mind when measuring the mass of a flywheel in the lab?

Yes, there are a few safety precautions to keep in mind when measuring the mass of a flywheel in the lab. First, be cautious when handling the flywheel as it may have sharp edges or moving parts. Also, always use proper protective gear, such as gloves and safety glasses, when handling weights. Finally, make sure to follow the instructions and guidelines provided by your lab instructor to ensure safe and accurate measurements.

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