What is the Tension in Block m2's String in a Pulley System?

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In a pulley system with two blocks, the tension in the string attached to block m2 is determined to be 2T, where T is the tension in the string attached to block m1. The force balance equations reveal that the acceleration of the blocks and the pulley must be considered, with the assumption of an ideal, massless pulley simplifying the analysis. The upward forces on block m2 consist of two tensions, leading to the conclusion that T2 equals 2T. The discussion emphasizes that for an ideal pulley, the net force approaches zero, confirming the relationship between the tensions in the strings. Understanding these dynamics is crucial for solving problems involving idealized pulley systems.
tzonehunter
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Homework Statement


The diagram shows a system of two blocks suspended by ideal strings and pulleys.
Pulleys_zps05b20a29.png

If the tension of the string attached to block m1 is T, what is the tension of the string attached to block m2?

Homework Equations


Due to conservation of string, a1/2 = a2
Force balance on mass 1:
∑F1 = m1a1 = m1g - T

Force balance on mass 2:
∑F2 = m2a2 = m2g - T2

The Attempt at a Solution


Substituting a1/2 = a2 into the ∑F2 expression, I get

a1 = 2g - 2T2/m2

Substituting the above into the ∑F1 expression, I get

T2 = m2g/2 + m2T/(2m1)

The correct answer is given as 2T. I'm struggling with this, because I don't see how the pulley could accelerate upwards if this is true, as all forces are balanced.
 
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The tension in the string is same since the string is assumed massless .It doesn't depend on the acceleration of the blocks .Since two strings are pulling block 2 upwards the upwards force on block 2 is 2T.
 
It may also be useful to note the tension across a frictionless pulley is uniform. So if you knew the tension on the left was ##T##, the tension in the two other strings is also ##T##. Since there is two of them, it is ##2T##.
 
tzonehunter said:

Homework Statement


T

Homework Equations


Due to conservation of string, a1/2 = a2
That is true for the magnitude of the accelerations. But they are of opposite directions. If m1 moves downward, m2 moves upward.
tzonehunter said:
Force balance on mass 1:
∑F1 = m1a1 = m1g - T
So you chose m1 moving downward.
tzonehunter said:
Force balance on mass 2:
∑F2 = m2a2 = m2g - T2

You have to change the sign of the right-hand side as m2 accelerates upward: m2a2 = T2-m2g

The tensions also act on the moving pulley, 2T upward and T2 downward. But the pulley is massless, so ma =0. The net force on the pulley must be zero.

ehild
 
Thank you to those that replied. I thought about this over night... I think I'm getting caught up in the idea that the pulley is a real object, but in the problem we're asked to assume an "ideal pulley".

How does this explanation sound:
The moveable pulley (subscript P) must have the same acceleration as m2. The acceleration of the moveable pulley is:
aP = FNet,P / mP = a2
FNet,P = 2T - T2

As long as m1 and m2 are constant, then a2 is constant and aP is constant.

An ideal pulley is massless, so as mP --> 0 , FNet,P --> 0. The lighter the pulley, the smaller the difference between 2T and T2. Less net force is required to produce the same acceleration of a less massive object.

This leaves us with

T2 --> 2T for the idealized case where mP --> 0.
 
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tzonehunter said:
Thank you to those that replied. I thought about this over night... I think I'm getting caught up in the idea that the pulley is a real object, but in the problem we're asked to assume an "ideal pulley".

How does this explanation sound:
The moveable pulley (subscript P) must have the same acceleration as m2. The acceleration of the moveable pulley is:
aP = FNet,P / mP = a2
FNet,P = 2T - T2

As long as m1 and m2 are constant, then a2 is constant and aP is constant. Indeed, if the pulley had non-negligible mass then you could not take the two upward tension forces as equal.

An ideal pulley is massless, so as mP --> 0 , FNet,P --> 0. The lighter the pulley, the smaller the difference between 2T and T2. Less net force is required to produce the same acceleration of a less massive object.

This leaves us with

T2 --> 2T for the idealized case where mP --> 0.
Yes. More generally, if an object is taken as massless then you can assume there's no net force on it (or its acceleration would be infinite). Similarly torques.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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