Problem with two pulleys and three masses

In summary, the conversation revolved around understanding the tension and weight distribution in a system involving masses and a pulley. It was concluded that in order for mass m1 to have no acceleration, the tension T1 in the string attached to m1 must be equal to m1*g. However, when mass M is zero, the tension in the string is also zero, and m1 will accelerate downwards at g. The conversation also touched upon Newton's law and the use of free body diagrams to understand the forces acting on each mass. Finally, an alternative approach was suggested involving finding the tension T(M,m2) in the string connecting the pulley to the ceiling and using this to solve for M when m1 is at rest.
  • #1
Erdi
37
6
Homework Statement
I cant figure out how to solve this task. I have got two pulleys, top pulley (A) and bottom pulley(B).
The pulley (A) is stuck to the wall and cannot move. The pulley B hangs in a thread and can
therefore moveup and down. Here m1 = 0.5 kg and m2 = 2.0 kg. Both pulleys can rotate freely. All
the pulleys can be are massless and there is no friction in the system.

How large must M be for m1 to be at rest?

Look at the figure.


Thanks for help!
Relevant Equations
T1 - m1g = ma, where a = 0
I know that the tension from pulley B (T1) has to be equal the m*g of m1 for m1 to have acceleration = 0. But i can't figure how this works because the m2 is already heavier. And so the block(M) has to be negative weight?
 
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  • #2
Heres the figure:
 

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  • #3
If M is zero which direction will m1 move? The problem is not a statics problem.
 
  • #4
If M is zero, and also the pulley(b) is massless. Then the only thing weighing on the right side would be m2 that is 2kg. So the m1 that is 0.5kg would move upwards right?
 
  • #5
What would (M=0) be the tension in the string if the pulleys are ideal and massless?
 
  • #6
Are you thinking of the tension on the string T1 (on m1 from pulley B) or the tension on the string T2 (on M from m2) For in both cases i would say it is (T = m2g = 2*9.81 = 19.64N)
 
  • #7
If M=0 then m1 will be accelerating down at g (there will be no constraint or T). If M is large then m1 will be accelerating up. Clearly somewhere in between m1 will have a=0
Draw a free body diagram for each mass and Newton for each . Put in the constraints from the pulley. Set a=0 for m1 (but not m2 m3)
 
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  • #8
I may be wrong here, but i think youre confusing m1 with m2. Because the constraint on m1 is affected by the pulley(B) which is again affected by both m2 and M. So if M is zero, the m2 will still be 2kg. So the m1 will still be constrained by m2 that is 2kg even though M = 0kg.
Also here is the free body diagram i drawed:
 

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  • #9
In the original figure the mass M seems to be heavier than m2, that is why the tension on m2 is larger than the tension on M in the diagram.
 
  • #10
The tension in a massless rope is everywhere the same.
There are only two ropes.
G is not force
 
  • #11
Erdi said:
So the m1 will still be constrained by m2 that is 2kg even though M = 0kg.
No. The rope will have no Tension
 
  • #12
Alright i kinda get it because T2 = Mg = 0*9.81 = 0.
But what happens to the m2 then? It has a mass, what about the tension from that object?
 
  • #13
It falls. "Tension from an object" is not a thing.
 
  • #14
Write down Newton for m2 and for M
 
  • #15
I drawed a new figure if M was to be 0 in this situation. But so what your conclusion is that fr m1 to stay at rest. In this situation M has to be 0 then?
Pull.JPG
 
  • #16
hutchphd said:
Write down Newton for m2 and for M
Newton for m2: 19.62N
Newton for M (if M is 0kg): 0
 
  • #17
No that is not what I said. Reread#7
Erdi said:
Newton for m2: 19.62N
Newton for M (if M is 0kg): 0
My apologies for my shorthand I meant write down Newton's Law for m2 and M
 
  • #18
hutchphd said:
No that is not what I said. Reread#7

My apologies for my shorthand I meant write down Newton's Law for m2 and M
So Newtons 2.law is F = ma
Where F will be T - mg, so it is T - mg = ma
But since M is zero, the tension will be 0
So it is -mg = ma
For M that is ofcourse 0, but i don't understand m2
-m2*g = mM*a => -m2*g = 0, so the tension here will also be 0?
 
  • #19
For whatever it's worth, here is a different approach.
  1. Assume that the pulley on the right is attached to the ceiling. Find the tension ##T(M,m_2)## in the string connecting it to the ceiling as a function of ##M##, ##m_2## and ##g##.
  2. Answer the question, "if ##m_1## is at rest, what must the tension ##T_1## be in the string attached to it?"
  3. Set ##T_1 = T(M,m_2)## and solve for ##M##.
 
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  • #20
kuruman said:
For whatever it's worth, here is a different approach.
  1. Assume that the pulley on the right is attached to the ceiling. Find the tension ##T(M,m_2)## in the string connecting it to the ceiling as a function of ##M##, ##m_2## and ##g##.
  2. Answer the question, "if ##m_1## is at rest, what must the tension ##T_1## be in the string attached to it?"
  3. Set ##T_1 = T(M,m_2)## and solve for ##M##.
T_1 has to be equal the m1*g => 4.905N
T_m2 = 2*9.81 = 19.64
T_M = x
T_1 = T_M * T_m2 => 4.905 = 19.64 * M
T_M = 4.905 / 19.64 = 0.25N = 0.025kg?
Or did you mean T_1 = T_M + T_m2?
In that case T_M = 4.905 - 19.64 = -14.73N = -1.5kg??
 
  • #21
It is correct to say that ##T_1=m_1g##. You missed my point for the rest of what you have to do. The picture below shows a massless pulley attached to the ceiling and two unequal masses ##M## and ##m_2##. The first step is to find an expression for tension ##T_2## in terms of ##m_2## and ##M##. The second step is to set the expression equal to ##m_1g## and solve for ##M##.

Atwood.png

On Edit:
Tension ##T_1## mentioned above is the tension in the piece of the rope that is attached to mass ##m_1## as defined in item 2, post #19. It is not tension ##T_1## shown in the figure above. I am sorry for the unfortunate choice of subscripts and the confusion it might cause.
 
Last edited:
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  • #22
I like @kuruman approach fine.
I note that the title of the thread is incorrect and belies the problem. This system is not in equilibrium. Just be aware of the mis-statement please.
 
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  • #23
Yea.. the title got corrected incorrectly by an admin. Anyway tho. If only look at the system with pulley B attatched to a rope and start finding an expression for T2 in terms of m2 and M. Isnt the expression just:
T2 = T(m2 + M) like you wrote down above? So that M = T2 - m2?
 
  • #24
Erdi said:
Yea.. the title got corrected incorrectly by an admin. Anyway tho. If only look at the system with pulley B attatched to a rope and start finding an expression for T2 in terms of m2 and M. Isnt the expression just:
T2 = T(m2 + M) like you wrote down above? So that M = T2 - m2?
I did not write T2=T(m2+M). I wrote ##T_2=T(M,m_2)##. This means "find ##T_2## as a function of ##m_2## and ##M##." When one writes ##f(x)=x^2+3x##, one does not mean ##fx=x^2+3x##.
 
  • #25
Oh my bad. Right i don't know why i didnt mention it before, but i know that's how i get solution to answer. The problem is, i have searched a lot around. But i can't find the formula for what the tension for T2 will be when we have two masses m2 and M. I have looked at several videos and other questions, but i can't find the specific solution to find that expression..
 
  • #26
Erdi said:
Oh my bad. Right i don't know why i didnt mention it before, but i know that's how i get solution to answer. The problem is, i have searched a lot around. But i can't find the formula for what the tension for T2 will be when we have two masses m2 and M. I have looked at several videos and other questions, but i can't find the specific solution to find that expression..
Can you find an expression for ##T_1## in the figure in post #21? If so, how do you think ##T_1## is related to ##T_2##?
 
  • #27
T1 = mg + ma. And i guess that T2 is equal to T1 because the rope and is massless and the pulley are frictionless or something? In that case, could you please try to just give a very understandable reason why it is equal.
 
  • #28
Erdi said:
T1 = mg + ma. And i guess that T2 is equal to T1 because the rope and is massless and the pulley are frictionless or something?
If ##m_1## is not accelerating, is the lower pulley accelerating vertically? What does the answer to that imply about the force balance on that lower pulley?
 
  • #29
erobz said:
If ##m_1## is not accelerating, is the lower pulley accelerating vertically? What does the answer to that imply about the force balance on that lower pulley?
If m1 isn't accelerating the lower pully can't be accelerating vertically. Which implies that the force balance on the lower pulley will be in equalibrium?
 
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  • #30
Erdi said:
If m1 isn't accelerating the lower pully can't be accelerating vertically. Which implies that the force balance on the lower pulley will be in equalibrium?
So the mass M is the same as m2 then?? M = 2kg?
 
  • #31
Erdi said:
So the mass M is the same as m2 then?? M = 2kg?
Slow down. You need some more things here. Do a FBD of the lower pulley. What are the forces acting on it? Remember you are isolating the pulley when you do this.
 
  • #32
The force acting on it will be T2 upward and m2 and M downwards
 

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  • #33
Erdi said:
The force acting on it will be T2 upward and m2 and M downwards
##m_2## or ##M## aren't forces. You are to be "freeing" the pulley from all other bodies, severing the ropes. What are the forces acting to pull the pulley down. What is the force acting to pull the pulley upward? Are these forces balanced on the pulley?
 
  • #34
erobz said:
##m_2## or ##M## aren't forces. You are to be "freeing" the pulley from all other bodies, severing the ropes. What are the forces acting to pull the pulley down. What is the force acting to pull the pulley upward? Are these forces balanced on the pulley?
If that's the case, forces acting on it downwards is the gravitational force. BUT i don't understand what you mean with the upward force. Because you said to isolate the pulley, but you agreed that it wasnt accelerating (vertically at least) so the upward force is the same as downward force then? which is the gravitatioal force ??
 
  • #35
Erdi said:
If that's the case, forces acting on it downwards is the gravitational force. BUT i don't understand what you mean with the upward force. Because you said to isolate the pulley, but you agreed that it wasnt accelerating (vertically at least) so the upward force is the same as downward force then? which is the gravitatioal force ??
We are freeing the pulley from the other bodies. Not from the forces. What are the internal forces inside the rope that we expose when we "free" the pulley.
 
<h2>1. What is the Problem with Two Pulleys and Three Masses?</h2><p>The problem with two pulleys and three masses is a classic physics problem that involves calculating the acceleration and tension in a system of pulleys and masses connected by strings or ropes. The problem is commonly used to demonstrate concepts such as Newton's laws of motion and the principles of conservation of energy and momentum.</p><h2>2. How do you approach solving this problem?</h2><p>To solve the problem with two pulleys and three masses, you first need to draw a free-body diagram of the system, identifying all the forces acting on each mass. Then, you can apply Newton's second law of motion to each mass to determine the acceleration. Next, use the principle of conservation of energy or momentum to find the unknown variables, such as the tension in the strings or the acceleration of the masses.</p><h2>3. What are the assumptions made in this problem?</h2><p>The problem with two pulleys and three masses assumes that the strings or ropes connecting the masses and pulleys are ideal and have no mass or friction. It also assumes that the pulleys are frictionless and massless. Additionally, the problem assumes that the masses are point masses and there is no air resistance.</p><h2>4. Can this problem be solved using different methods?</h2><p>Yes, this problem can be solved using different methods, such as using the principles of rotational motion or using vector algebra. However, the most common approach is to use Newton's laws of motion and the principles of conservation of energy or momentum.</p><h2>5. What are some real-life applications of this problem?</h2><p>The problem with two pulleys and three masses has many real-life applications, such as in engineering, where it can be used to design and optimize pulley systems for lifting and moving heavy objects. It is also relevant in physics and mechanics, where it can be used to understand the motion of objects connected by strings or ropes, such as in a simple pendulum or a block and tackle system.</p>

1. What is the Problem with Two Pulleys and Three Masses?

The problem with two pulleys and three masses is a classic physics problem that involves calculating the acceleration and tension in a system of pulleys and masses connected by strings or ropes. The problem is commonly used to demonstrate concepts such as Newton's laws of motion and the principles of conservation of energy and momentum.

2. How do you approach solving this problem?

To solve the problem with two pulleys and three masses, you first need to draw a free-body diagram of the system, identifying all the forces acting on each mass. Then, you can apply Newton's second law of motion to each mass to determine the acceleration. Next, use the principle of conservation of energy or momentum to find the unknown variables, such as the tension in the strings or the acceleration of the masses.

3. What are the assumptions made in this problem?

The problem with two pulleys and three masses assumes that the strings or ropes connecting the masses and pulleys are ideal and have no mass or friction. It also assumes that the pulleys are frictionless and massless. Additionally, the problem assumes that the masses are point masses and there is no air resistance.

4. Can this problem be solved using different methods?

Yes, this problem can be solved using different methods, such as using the principles of rotational motion or using vector algebra. However, the most common approach is to use Newton's laws of motion and the principles of conservation of energy or momentum.

5. What are some real-life applications of this problem?

The problem with two pulleys and three masses has many real-life applications, such as in engineering, where it can be used to design and optimize pulley systems for lifting and moving heavy objects. It is also relevant in physics and mechanics, where it can be used to understand the motion of objects connected by strings or ropes, such as in a simple pendulum or a block and tackle system.

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