Finding Equilibrium State for Two Blocks Connected by Pulley System

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Homework Help Overview

The discussion revolves around a physics problem involving two blocks connected by a pulley system. The original poster seeks to determine the conditions under which the system comes to rest and the maximum distance one of the blocks will fall. The setup includes specified masses and an initial distance between the blocks, with the block on the right being released to slide down a frictionless surface.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants discuss various methods for analyzing the problem, including force-work relationships and energy conservation principles. The original poster expresses confusion over the complexity of their energy-based approach and questions when to apply different methods. Others suggest that the system may oscillate and question the assumption of energy conservation due to the lack of friction.

Discussion Status

The conversation is ongoing, with participants exploring different interpretations of the problem. Some have offered insights into the energy dynamics of the system, while others are questioning the assumptions made regarding friction and energy conservation. There is no explicit consensus yet on the best approach to take.

Contextual Notes

Participants note that the problem may require a reevaluation of the initial conditions and assumptions, particularly regarding the presence of friction and the nature of the system's motion. The original poster acknowledges a potential misunderstanding in their initial question, which may affect the direction of the discussion.

TheFerruccio
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Two Blocks Connected by Pulley System

Homework Statement



[EDIT] sorry, I forgot to post the goal of this problem.
[EDIT] I wrote the question wrong.
At what point does the system come to rest?

What is the maximum distance it will fall?

Two blocks are connected by a rope and pulley system. The block on the right is released and is allowed to slide down the frictionless surface. The masses are specified, and their initial distance apart.

Homework Equations


This is where I have the question. But, here are some diagrams that I made showing what I mean.
siBI3cH.png

2CaWpkt.png


The Attempt at a Solution



I have tried approaching it from two different methods.

1: Force-work relationships and momentum
2: Energy relationshipsI end up getting stuck in my attempts to solve this problem. It is deceptively simple, and I keep telling myself that it has a simple answer.

Let me give you the energy example of what I tried to do.

I said that the energy of the system must always be conserved, from the point of release to its energy equilibrium state. Thus, the sum of the potential and kinetic energies of both systems must equal.

I denoted a new constant, k, representing the length of the diagonal of the wire. I also denoted an angle from k to the diagonal, Θ. I found the vertical displacement of the left mass as k-a. The right mass has a vertical displacement d, which also relates to Θ.

So, my initial equation is:
Initial energy = 0 (what I defined as my 0 energy state, since I only care about the change of potential energy of the two masses)

0 = 2mg(k-a)-mgd-0.5(2m)\dot{k}^2+0.5m\dot{d}^2

This seems to get rather complicated fast. I can parameterize both k and d as:

d=k\sin{\theta}
and
\dot{d}=\dot{k}\sin{\theta}+k\cos{\theta}\dot{\theta}But, I am getting stuck from here. This seems to be exploding in complexity from something so simple. Is there a better, more elegant way to approach this?

I might be coming back with further questions, because I still do not have a solid grasp of when itis best to use force/momentum, or potential/kinetic energy when I am approaching these problems. I do not have a good grasp of when it is conserved and when it isn't. For instance, in this problem, since there are no impacts, and the problem seems to lack a distinct before/after to it, the energy of the system is conserved, which is why I tried to approach it from the energy perspective.

Should I use both methods to resolve some of the complexity? I do not have a good grasp of this. All of the class notes consist of very pure theory and vector analysis, so I have yet to strongly link the class notes to the actual applications.
 
Last edited:
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TheFerruccio said:

Homework Statement



[EDIT] sorry, I forgot to post the goal of this problem.

At what point does the system come to rest?

Two blocks are connected by a rope and pulley system. The block on the right is released and is allowed to slide down the frictionless surface. The masses are specified, and their initial distance apart.

Homework Equations


This is where I have the question. But, here are some diagrams that I made showing what I mean.
siBI3cH.png

2CaWpkt.png


The Attempt at a Solution



I have tried approaching it from two different methods.

1: Force-work relationships and momentum
2: Energy relationshipsI end up getting stuck in my attempts to solve this problem. It is deceptively simple, and I keep telling myself that it has a simple answer.

Let me give you the energy example of what I tried to do.

I said that the energy of the system must always be conserved, from the point of release to its energy equilibrium state. Thus, the sum of the potential and kinetic energies of both systems must equal.

I denoted a new constant, k, representing the length of the diagonal of the wire. I also denoted an angle from k to the diagonal, Θ. I found the vertical displacement of the left mass as k-a. The right mass has a vertical displacement d, which also relates to Θ.

So, my initial equation is:
Initial energy = 0 (what I defined as my 0 energy state, since I only care about the change of potential energy of the two masses)

0 = 2mg(k-a)-mgd-0.5(2m)\dot{k}^2+0.5m\dot{d}^2

This seems to get rather complicated fast. I can parameterize both k and d as:

d=k\sin{\theta}
and
\dot{d}=\dot{k}\sin{\theta}+k\cos{\theta}\dot{\theta}But, I am getting stuck from here. This seems to be exploding in complexity from something so simple. Is there a better, more elegant way to approach this?

I might be coming back with further questions, because I still do not have a solid grasp of when itis best to use force/momentum, or potential/kinetic energy when I am approaching these problems. I do not have a good grasp of when it is conserved and when it isn't. For instance, in this problem, since there are no impacts, and the problem seems to lack a distinct before/after to it, the energy of the system is conserved, which is why I tried to approach it from the energy perspective.

Should I use both methods to resolve some of the complexity? I do not have a good grasp of this. All of the class notes consist of very pure theory and vector analysis, so I have yet to strongly link the class notes to the actual applications.

Looks to me like a force problem. The blocks can be at rest when the tension in rope balances the force of gravity on the smaller block. If you just release the system in it's initial state and there is no friction at all, then it will never come to rest. It will just oscillate. So I think you need to assume there is some friction someplace (even if it's not on the surface). That would make assuming energy conservation a bad idea. Or am I making it too simple?
 
That was my first assumption when looking at the problem, that the system would oscillate and never come to rest.
Dang, you know what, I asked the question wrong, and I might have to redo the whole thread so other readers can see what I said.

The actual question was "What is the maximum distance it will fall?" in which case it is asking for the lowest point the block will go.

Alright, then, how does one set up the differential equation for this? I really am still at a loss, even with that information.
 
TheFerruccio said:
The actual question was "What is the maximum distance it will fall?" in which case it is asking for the lowest point the block will go.

Alright, then, how does one set up the differential equation for this? I really am still at a loss, even with that information.

Think about energy. What is the KE at the lowest point?
 
TheFerruccio said:
That was my first assumption when looking at the problem, that the system would oscillate and never come to rest.
Dang, you know what, I asked the question wrong, and I might have to redo the whole thread so other readers can see what I said.

The actual question was "What is the maximum distance it will fall?" in which case it is asking for the lowest point the block will go.

Alright, then, how does one set up the differential equation for this? I really am still at a loss, even with that information.

You don't need a differential equation. Use energy. Define the initial PE to be zero. Since KE+PE is conserved and you start with KE=0, when they momentarily at rest at the end of the fall then KE=0 again. So PE must be zero again. Where can that happen?
 
Dick said:
You don't need a differential equation. Use energy. Define the initial PE to be zero. Since KE+PE is conserved and you start with KE=0, when they momentarily at rest at the end of the fall then KE=0 again. So PE must be zero again. Where can that happen?

When the lighter block falls, it moves down a distance d, losing a potential energy mgd. The larger block must lift up by the same energy change, since this is a conservative system.

Thus mgd=2mgx, then the larger block moves up half the distance that the smaller block moves down. However, I do not know how to find the magnitude of this movement.
 
TheFerruccio said:
When the lighter block falls, it moves down a distance d, losing a potential energy mgd. The larger block must lift up by the same energy change, since this is a conservative system.

Thus mgd=2mgx, then the larger block moves up half the distance that the smaller block moves down. However, I do not know how to find the magnitude of this movement.

That's just geometry. When the block has descended distance d, what is the distance from it to the pulley?
 
haruspex said:
That's just geometry. When the block has descended distance d, what is the distance from it to the pulley?

There is probably a higher level conceptual understanding that I am missing here.

The distance from the pulley is \sqrt{a^2+d^2} But, the goal is to completely eliminate d altogether and express it fully in terms of the given information (the masses, a, gravity if applicable...) I am definitely not thinking this through properly.

I'm thinking, maybe,

\sqrt{a^2+d^2}=a+\frac{d}{2} Then I can solve for d in this manner.

This yields a d = 4/3 a

Ah ha! Thanks for the help. You're right. It was just geometry. I was just getting stuck on how to see it.
 
Last edited:

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