Newton`s 3rd Law Tension Solved Question

In summary: The tension in the top segment would be 5*2=10, since the top segment has tension in it from both the left and right ropes. However, the left and right segments together only weigh 10, so the pulley only moves an extra 5 units. The pulley therefore only moves an extra 2.5 units to the right, not 5.2) is correct.
  • #1
Sabellic
68
0

Homework Statement



http://img511.imageshack.us/img511/8721/problem1ldc0.jpg

Homework Equations


They are listed in the image above, but it`s all rooted in the basic Tension equation:
F-Ft=ma

The Attempt at a Solution


This is a different question I am asking. The problem IS solved as you can see. But I am having trouble understanding the logic behind it.

The writers say that mass 1 has twice the acceleration as mass 2. They totally lost me there. Why is that the case? And how do I interpret it from the image? And then they say that when the pulley moves a distance d, m1 moves 2d. Once again, I`m clueless as to why that is. And when they say the pulley moves, they mean the pulley is moving rather than rotating, right? But either way, I lost the point. Why will m1 move distance of 2d? Wouldn`t that entail it going ahead of the pulley, or will the rope pulling it make it come in contact with the pulley?

Then they say, the tension in Ft1 is half that of Ft2. Why?? How did they arrive at that observation? I cannot interpret the reason from regarding the image alone. Why would the total force on the pulley being zero make Ft1 have less tension??

Somebody please help me.
 
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  • #2
Sabellic said:
The writers say that mass 1 has twice the acceleration as mass 2. They totally lost me there. Why is that the case? And how do I interpret it from the image? And then they say that when the pulley moves a distance d, m1 moves 2d. Once again, I`m clueless as to why that is. And when they say the pulley moves, they mean the pulley is moving rather than rotating, right? But either way, I lost the point. Why will m1 move distance of 2d?
Yes, when they talk about the pulley moving, they mean its center moving sideways. Note that the pulley and mass 2 are connected, so they move together.

The best way to understand how the rope/pulley arrangement constrains the motion of the masses is to take a piece of string and play around with it. Since the string is doubled over the pulley, mass 1 must move twice as fast as mass 2.

Another way to look at it is to examine the rope wrapped around the pulley. Think of it as having two parts: the top side and the bottom side. If the pulley moves 1 foot to the right, the top side lengthens by 1 foot. Since the rope's length is fixed, that means the bottom section must shorten by 1 foot, making m1 closer to the pulley by 1 foot. So... the pulley has moved to the right by 1 foot and m1 is closer to the pulley by 1 foot... thus m1 must have moved a net distance of 2 feet to the right. Make sense?

Wouldn`t that entail it going ahead of the pulley, or will the rope pulling it make it come in contact with the pulley?
Sooner or later m1 will bang into the pulley--and then the party's over for this little set up! :smile: (Pretend that it never gets that far.)

Then they say, the tension in Ft1 is half that of Ft2. Why?? How did they arrive at that observation? I cannot interpret the reason from regarding the image alone. Why would the total force on the pulley being zero make Ft1 have less tension??
Each rope segment attached to the pulley exerts a force on the pulley. The left rope attaches twice, so it exerts its tension twice. That force is balanced by the single right rope segment, so it must exert twice the tension.

Realize that these effects are connected. Since the rope/pulley constrains the system so that m2 only moves half as far as m1, it must exert twice the force to conserve energy.
 
  • #3
Doc Al, I can`t thank you enough for the attention you gave to this. I`m still milling your explanation around in my head, but you addressed everything very well for me.

So, basically m1 moves twice as much because it:
1) Moves the same distance as the pulley.
2) The tension from Ft1 pulls on the rope attached to m1 and the length of the bottom part of the rope diminishes.

Correct?
 
  • #4
I think you're getting it, but allow me to restate it a bit. M1 moves twice as fast as M2 (which moves at the same speed as the pulley) since:
(1) M1 gets closer to the pulley at the same rate as the pulley moves
(2) the pulley itself moves

When you add these two speeds you'll see that M1 must move twice as fast as M2.
 
  • #5
1) is NOT correct.

Look at the top segment of the rope, ending right in front of the pulley (a straight line segment plus a quarter circle:
Suppose the pulley moves some distance D forward.
Then, the top segment of the rope still consists of a quarter circle and a straight line sgment.
Clearly, since the arc length of the quarter circle does not change, and the top segment is fixed to the wall, its end unmoving, it means that the straight line segment of the top rope piece must have increased with a length D. Otherwise, the pulley wouldn't be able to move a distance D forward, contradicting the hypothesis.

Now, the lengthening of the top segment cannot be in the form of a stringlike stretching; a rope is considered to be of FIXED length.

Hence, that increase in length of the top piece of the rope can only come about if the lower rope straight line segment has SHORTENED by a length D.

Now, if m1 had only moved the same distance as the pulley, then the relative distince between them, would remain constant.
But that relative distance is, precisely, determined by the length of the lower rope's straight line segment!

Hence, m1 must move twice the distance D as the pulley, in order to decrease the lower rope's straight line part with length D.

Thus, the acceleration of m1 must be twice that of the pulley, and therefore twice that of m2, since the pulley and m2 has the same acceleration.
 
  • #6
arildno said:
1) is NOT correct.
Say what?

Look at the top segment of the rope, ending right in front of the pulley (a straight line segment plus a quarter circle:
Suppose the pulley moves some distance D forward.
Then, the top segment of the rope still consists of a quarter circle and a straight line sgment.
Clearly, since the arc length of the quarter circle does not change, and the top segment is fixed to the wall, its end unmoving, it means that the straight line segment of the top rope piece must have increased with a length D. Otherwise, the pulley wouldn't be able to move a distance D forward, contradicting the hypothesis.

Now, the lengthening of the top segment cannot be in the form of a stringlike stretching; a rope is considered to be of FIXED length.

Hence, that increase in length of the top piece of the rope can only come about if the lower rope straight line segment has SHORTENED by a length D.
This is exactly what I stated. Reread what I wrote:
(1) M1 gets closer to the pulley at the same rate as the pulley moves​
 
  • #7
1) was a reference to Sabelle's misstatement "1) Moves the same distance as the pulley."

I need time to write my reply, yours wasn't up when I began it..:smile:
 
  • #8
arildno said:
1) was a reference to Sabelle's misstatement "1) Moves the same distance as the pulley."
D'oh! :uhh: (Next time please use quotes!)

arildno said:
I need time to write my reply, yours wasn't up when I began it..:smile:
That's happened to me a few too many times. :redface:
 

1. What is Newton's 3rd Law?

Newton's 3rd Law, also known as the law of action and reaction, states that for every action, there is an equal and opposite reaction. This means that when one object exerts a force on another object, the second object will exert an equal and opposite force back on the first object.

2. How does Newton's 3rd Law relate to tension?

Newton's 3rd Law applies to tension in the sense that when an object applies a force on a string or rope, the string will also apply an equal and opposite force on the object. This creates tension in the string, which can be calculated using Newton's 3rd Law equation.

3. What is the formula for calculating tension using Newton's 3rd Law?

The formula for calculating tension using Newton's 3rd Law is T = F, where T is the tension in the string, and F is the force applied on the object by the string. This formula assumes that the string is in equilibrium, meaning that the forces acting on it are balanced.

4. Can Newton's 3rd Law be used to solve tension problems?

Yes, Newton's 3rd Law can be used to solve tension problems, as it provides a way to calculate the tension in a string or rope when the forces acting on it are known. By using the formula T = F, the tension can be determined and used to solve other related problems.

5. Are there any real-life applications of Newton's 3rd Law and tension?

There are many real-life applications of Newton's 3rd Law and tension, such as in bridges, cranes, and elevators. These structures use tension to balance the forces acting on them and prevent them from collapsing. Additionally, tension is also used in sports equipment, such as tennis rackets and trampolines, to provide the necessary force for the objects to work properly.

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