Solving for Acceleration in a Pulley System

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Homework Help Overview

The problem involves a painter and a scaffold connected by ropes over pulleys, where the painter pulls himself up with a force while accelerating upwards. The goal is to find the acceleration of the system, considering the masses of both the painter and the scaffold.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss various equations of motion for the painter and scaffold, questioning the application of Newton's laws and the relationships between forces. Some participants express confusion over the normal forces and their interactions, while others attempt to derive equations for acceleration based on different assumptions.

Discussion Status

Several participants have provided insights and corrections regarding the equations used, noting potential sign errors and misunderstandings of force interactions. There is ongoing exploration of the relationships between the forces acting on the painter and the scaffold, with no clear consensus reached yet.

Contextual Notes

Participants are working under the constraints of a homework assignment, which may limit the information they can use or the assumptions they can make. The discussion includes questioning the validity of certain assumptions, such as the equality of normal forces and the implications of mass ratios on the system's behavior.

Radarithm
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Homework Statement



A painter of mass M stands on a scaffold of mass m and pulls himself up by two ropes which hang over pulleys, as shown. He pulls each rope with a force F and accelerates upwards with a uniform acceleration a. Find a - neglecting the fact that no one could do this for long.

Homework Equations



F=M\ddot{y}
\zeta=(M+m)
F=\zeta\ddot{y}
For the painter:
2T-N_1-Mg=M\ddot{y}
For the scaffold alone:
2T-mg-N_2=m\ddot{y}
For the entire system:
T_\Sigma -\zeta g=\zeta\ddot{y}

The Attempt at a Solution


I have assumed that:
1 - N_2=Mg because of Newton's 3rd Law.
2 - The acceleration of the entire system is \ddot{y}.

After solving for numerous equations, I checked the solutions section and got a hint: if M=m then a=g. After plugging in values, I did not get g but instead 2g and many other values. My first approach:

Entire system: T_\Sigma -\zeta g=\zeta\ddot{y}
So T_\Sigma=\zeta(g+\ddot{y}) and \ddot{y}=T_\Sigma -g=2F-g
For the painter: 2F-N_1-Mg=M\ddot{y}. Since N_1=Mg, that means that:
\zeta (g+\ddot{y})=M\ddot{y} which leads to: \ddot{y}(M-\zeta)=\zeta g. Solving for the acceleration, we get: \ddot{y}=\frac{\zeta g}{(M-\zeta)}.
When I let M and m equal 1, I got twice the acceleration. Where did I go wrong? I had many more attempts but this one seems like the clearest one to me.
 
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1st, there is a sign mistake in the equation for the painter

2nd, your application of the 3rd law makes no sense. Those forces are not a pair of action and reaction. One is a normal force and the other is a gravitational force. A pair of action and reaction will always have the same nature. Pair normal with normal and gravity with gravity. Also the pair of forces never-ever-ever act on the same object. It's always Object A acts on object B and object B reacts on object A.
 
Radarithm said:
For the painter:
2T-N_1-Mg=M\ddot{y}
For the scaffold alone:
2T-mg-N_2=m\ddot{y}
Isn't ##N_1## the normal force of the scaffold acting on the painter? It should be upward. Also, if ##N_2## is the normal force of the painter on the scaffold, then ##N_1 = N_2##.
I have assumed that:
1 - N_2=Mg because of Newton's 3rd Law.
As noted above, ##N_1 = N_2##, but I don't see why these would be equal to ##Mg## (the weight of the painter). Indeed, if ##M < m## then there won't be any contact force at all.
 
[STRIKE][/STRIKE]I was able to derive a second equation, but I get 6.2 m/s^2:
Painter: 2F+N_1-Mg=M\ddot{y}
Scaffold alone: 2F-N_2-mg=m\ddot{y}

N_2=N_1
N_2=2F-m(g-\ddot{y})

System itself: F-\zeta g=\zeta\ddot{y}

T-\zeta g=\zeta\ddot{y}
2F=\zeta (g+\ddot{y})

This means that if I plug this into the equation for the painter:
2\zeta(g+\ddot{y})-g(m-M)=\ddot{y}(M+m)
M\ddot{y}+m\ddot{y}+2\zeta\ddot{y}=g(2\zeta -m-M)
\ddot{y}(M+m+2\zeta)=g(2\zeta -m-M)
g\frac{(2\zeta -m-M)}{(M+m+2\zeta)}

The mistake is staring me right in the face. :confused:
 
Radarithm said:
[STRIKE][/STRIKE]I was able to derive a second equation, but I get 6.2 m/s^2:
Painter: 2F+N_1-Mg=M\ddot{y}
Scaffold alone: 2F-N_2-mg=m\ddot{y}

N_2=N_1
N_2=2F-m(g-\ddot{y})
Already you've made a sign error in that last equation, assuming it is supposed to be a rearrangement of the "scaffold alone" equation above.
 
Also, the equation 2F=ζ(g+y¨) for the whole system is wrong. The left side is off by a factor of 2.
 
So I think this post is dead but I'll give it a shot and try to revive it. I'm sorry if it seems inappropriate but I must also check my answer to this problem

Here is my my analysis:

##2T+N_{scaffold}-M_{parinter}g=M_{painter}a_{painter}##

##2T-N_{painter}-m_{scaffold}g=m_{scaffold}a_{scaffold}##

since ##a_{painter}=a_{scaffold}## and ##N_{painter}=N_{scaffold}## and we can solve for simply ##a## (acceleration of the painter and scaffold) by adding the equations and diving by ##M+m##

##a=\frac{4T-(M+m)g}{M+m}##

Now it turns weird. I can assume by Newton's Third Law that ##F## of the painter should create an equal and opposite tension on the rope, yielding

##a=\frac{4F-(M+m)g}{M+m}##

which agrees with the clue given in the book, but I'm a little hesitant with this since I feel the scaffold (and the painter just by standing on it) must somehow also be affecting the tension.

Any help?
 
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