Solid Disk Pulley + 2 Mass system, v derivation using 2 methods

In summary: I'm fairly confident in my solution now. :)I think I understand the process a little better now. Thank you very much!In summary, the conversation discusses a problem involving velocity and energy equations, with a focus on using the Conservation of Energy equations to replicate the velocity equation. The individual asking the question has arrived at two different answers using energy conservation and is seeking clarification on which is correct. The conversation concludes with an explanation of how to correctly use energy conservation to solve the problem and a reminder to not rely on previous incorrect results.
  • #1
Dorian
10
1

Homework Statement



[please see attached photo]

Homework Equations



[please see attached photo]

The Attempt at a Solution



[please see attached photo]

The issue for me starts with (but probably doesn't end with) replicating the velocity equation using the Conservation of Energy equations. Is this Second Law derived equation correct to begin with? I've tried and have arrived at a few different answers using the Conservation of Energy equations. One was V=(gh)^(1/2). Another was V=(2gh/3)^(1/2).

edit: Oh, shoot. You may have to zoom in for the relevant equations. My apologies :(
 

Attachments

  • sir problem_zer equassians_my attempt.png
    sir problem_zer equassians_my attempt.png
    29.1 KB · Views: 339
Physics news on Phys.org
  • #2
Hi Dorian and welcome to PF.

Can you show your two different solutions using energy conservation? Your solution using dynamics has a problem. The first equation in (b) should result in ##T_2=\frac{3}{2}mg\sin \theta-3ma##. You forgot to carry the sine through.
 
  • #3
kuruman said:
Hi Dorian and welcome to PF.

Can you show your two different solutions using energy conservation? Your solution using dynamics has a problem. The first equation in (b) should result in ##T_2=\frac{3}{2}mg\sin \theta-3ma##. You forgot to carry the sine through.
I didn't carry it because ##T_2=3mg\sin \theta-3ma=3mg\sin(30)-3ma=\frac{3}{2}mg-3ma##
 
  • #4
OK, thanks for the clarification. Then your answer in (b) should be correct. What about energy conservation? Can you show how you got your different answers?
 
  • #5
kuruman said:
OK, thanks for the clarification. Then your answer in (b) should be correct. What about energy conservation? Can you show how you got your different answers?

Sure thing! Thank you for the prompt responses, by the way. :)

I think the issue for me arises in the potential energy. For the right side of the equation, I have ##\frac{1}{2}3mv^{2}+\tfrac{1}{2}mv^{2}+\frac{1}{2}(\frac{1}{2}2mR^{2})(\frac{v^{2}}{R^{2}})=\frac{5mv^{2}}{2}##. But the right side leaves me to believe I should have mgh on the left side. I don't understand how. 3mgh-2mgh, perhaps? I don't know.
 
  • #6
Dorian said:
But the right side leaves me to believe I should have mgh on the left side. I don't understand how. 3mgh-2mgh, perhaps? I don't know.
Yes you need to add potential energy terms it doesn't matter on which side because the zero of potential energy is arbitrary. So let's say that the potential energy is zero at the point where they are released from rest. Then ##U_i=0## on the left side. For the right side, note that the hanging mass gains potential energy while the mass on the incline loses potential energy. Then ##U_f=mgh_1-3mgh_2##. Now ##h_2=h## as shown in the figure, but ##h_1 \neq h##. Put it together.
 
  • #7
kuruman said:
Yes you need to add potential energy terms it doesn't matter on which side because the zero of potential energy is arbitrary. So let's say that the potential energy is zero at the point where they are released from rest. Then ##U_i=0## on the left side. For the right side, note that the hanging mass gains potential energy while the mass on the incline loses potential energy. Then ##U_f=mgh_1-3mgh_2##. Now ##h_2=h## as shown in the figure, but ##h_1 \neq h##. Put it together.

edit: I think I figured it out:
##h_{1}=\Delta s##
and
##sin(30^{\circ})=\frac{h}{\Delta s}\rightarrow {\Delta s}=\frac{h}{sin(30^{\circ})}=2h##

As such,
##PE_{0}=PE=3mgh=mg\Delta s\rightarrow 3mgh-mg\Delta s=3mgh-mg(2h)=3mgh-2mgh=mgh##

Now for Conservation of Energy (as simplified earlier):
##mgh=\frac{5}{2}mv^{2}\rightarrow v=\sqrt{\frac{2gh}{5}}##

Please let me know if this makes sense.
 
Last edited:
  • #8
Your treatment of potential energy doesn't make sense. Especially the equality ##PE_0=PE## What do these two stand for and why are they equal? Where is your zero of potential energy?
I suggest that you start by writing the energy conservation equation at two points: point A is the starting point from rest and point B is where mass ##3m## has dropped a vertical distance ##h## and mass ##m## has risen vertical distance ##2h##. Assume that the potential energy at point A is ##PE_A=0##. Since the system starts from rest, ##KE_A =0##. By energy conservation, ##KE_B+PE_B=0## as well. At this point you need to find expressions for ##KE_B## and ##PE_B##, substitute and solve for the speed ##v##.
Dorian said:
Now for Conservation of Energy (as simplified earlier):
As a matter of good habit I would recommend against using previous results unless you are 100% certain that they are correct to avoid propagating mistakes. Restart from the beginning, preferably using a different path.
 
  • #9
kuruman said:
Your treatment of potential energy doesn't make sense. Especially the equality ##PE_0=PE## What do these two stand for and why are they equal? Where is your zero of potential energy?
I suggest that you start by writing the energy conservation equation at two points: point A is the starting point from rest and point B is where mass ##3m## has dropped a vertical distance ##h## and mass ##m## has risen vertical distance ##2h##. Assume that the potential energy at point A is ##PE_A=0##. Since the system starts from rest, ##KE_A =0##. By energy conservation, ##KE_B+PE_B=0## as well. At this point you need to find expressions for ##KE_B## and ##PE_B##, substitute and solve for the speed ##v##.

As a matter of good habit I would recommend against using previous results unless you are 100% certain that they are correct to avoid propagating mistakes. Restart from the beginning, preferably using a different path.

They're from the Conservation of Energy equation, and what you stated is precisely what I did. I'm sorry you didn't interpret it the way I intended it to be interpreted. What I provided wasn't the complete product, merely me looking for a comment on if this part of my derivation made sense, not the entire picture.

##PE_{0}## is the initial potential energy of the system. ##PE## is the final potential energy of the system. The same logic follows for initial kinetic energy ##KE_{0}## and final kinetic energy ##KE##. I eschewed a few steps that I had written down already in the hopes that I wouldn't have needed to provide them since it was already discussed. I'm sorry, sincerely.

My reference height for ##mass_{2}=3m## is its ending point. My reference height for ##mass_{1}=m## is its starting point.

The entire formula for the system is

##PE_{0}+KE_{0}=PE+KE##,

which is

##\ PE_{m2}=PE_{m10}=KE_{m10}=KE_{m20}=0 \\ PE_{m20}=3mgh\ ,\ PE_{m1}=mg(2h)\ ,\ KE_{m1}=\frac{1}{2}mv^{2}\ ,\ KE_{m2}=\frac{1}{2}(3m)v^{2}\ ,\ KE_{rot}=\frac{1}{2}\mathbb{I} \omega^{2}=\frac{1}{2}(2mR^{2})(\frac{v^{2}}{R^{2}})##

##3mgh=mg(2h)+\frac{1}{2}(3m)v^{2}+\frac{1}{2}mv^{2}+\frac{1}{2}(2mR^{2})(\frac{v^{2}}{R^{2}})##
 
  • #10
Your last equation is correct, but I am not convinced that you know what you are doing as opposed to cooking up an equation that gives you the answer that you know is correct. Your expression for the total kinetic energy is correct. Now assume that zero potential energy is at the starting point. This means (in your notation) that ##PE_{m10} = 0## and ##PE_{m20} = 0## so that ##PE_0 = PE_{m10}+PE_{m20}=0## is the initial potential energy. The initial kinetic energy is zero so that the initial mechanical energy, ##ME_0=PE_0+KE_0=0##, is also zero.

Energy conservation demands that the final mechanical energy must equal the initial mechanical energy, ##ME=PE+KE=0##.
You have correctly found the final kinetic energy to be
##KE=\frac{1}{2}(3m)v^{2}+\frac{1}{2}mv^{2}+\frac{1}{2}(2mR^{2})(\frac{v^{2}}{R^{2}})##
What is the correct expression for the final potential energy ##PE~##?
 
  • #11
kuruman said:
but I am not convinced that you know what you are doing as opposed to cooking up an equation that gives you the answer that you know is correct.

Goodness. That was a little condescending and I've been nothing but respectful toward you. :/

In anyway event, I used different reference heights for the two masses. If I gave both ##PE_{m10}## and ##PE_{m20}## zero potential energy for both of their starting positions, then the final potential energy, ##PE_{m1}## and ##PE_{m2}## would be ##mg(2h)## and ##-3mgh##, respectively.

So, ##PE=mg(2h)-3mgh##
 
  • #12
Dorian said:
Goodness. That was a little condescending and I've been nothing but respectful toward you. :/

In anyway event, I used different reference heights for the two masses. If I gave both ##PE_{m10}## and ##PE_{m20}## zero potential energy for both of their starting positions, then the final potential energy, ##PE_{m1}## and ##PE_{m2}## would be ##mg(2h)## and ##-3mgh##, respectively.

So, ##PE=mg(2h)-3mgh##
That's it, you got it! :smile: I meant no disrespect, and I am sorry if you thought I did.
 
  • #13
kuruman said:
That's it, you got it! :smile:

Apology accepted. =) I am truly appreciative of your prompt responses and your help. Thank you, sincerely. :smile:
 
Last edited:

FAQ: Solid Disk Pulley + 2 Mass system, v derivation using 2 methods

1. What is a solid disk pulley?

A solid disk pulley is a type of pulley that consists of a circular disk with a groove around its circumference. The groove is used to hold a rope or belt, which is used to transmit rotational motion or force.

2. How does a 2 mass system work with a solid disk pulley?

In a 2 mass system, there are two masses connected by a rope or belt that runs over a solid disk pulley. When one mass is lifted or pulled, the other mass will move in the opposite direction due to the conservation of energy.

3. What are the two methods used to derive the velocity of a solid disk pulley + 2 mass system?

The two methods used to derive the velocity are the Newton's Second Law method and the Work-Energy Theorem method. Both methods use the principles of classical mechanics to determine the velocity of the system.

4. What is the Newton's Second Law method for deriving the velocity?

The Newton's Second Law method uses the equation F=ma, where F is the net force acting on the system, m is the mass of the system, and a is the acceleration. By applying this equation to the system, the velocity can be determined.

5. How does the Work-Energy Theorem method derive the velocity of a solid disk pulley + 2 mass system?

The Work-Energy Theorem method uses the principle of conservation of energy, which states that the total energy of a system remains constant. By equating the work done on the system to the change in kinetic energy, the velocity can be calculated.

Similar threads

Replies
40
Views
3K
Replies
3
Views
1K
Replies
22
Views
4K
Replies
3
Views
919
Replies
30
Views
2K
Replies
13
Views
3K
Back
Top