Why Does Tension Act in Two Directions at a Point in a String?

AI Thread Summary
Tension in a string acts in two directions at any point due to the nature of forces being transmitted through the string. When a string is pulled from both ends, it remains taut, demonstrating that tension is a pulling force that balances the system. In the case of a pulley, tension can be analyzed by considering the forces acting on it; if the pulley is massless, the tensions must balance, but if it has mass, the net force must account for gravity, leading to different tensions acting on either side. The discussion highlights that while tension pulls in both directions, the net effect on the pulley can lead to movement depending on the overall forces involved. Understanding these dynamics is crucial for analyzing systems involving pulleys and strings.
andyrk
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Why is tension at a specific point in a string in 2 directions? For example in the first part of image 1, the string is pulling the two blocks upwards. And in the second part of image 1, the string is pulling the pulley down too. Does tension at a point in a string try to pull the point in 2 directions?

And in image 2, why is the bottom most pulley (which is not hinged) pulled up by a tension 2T? If it is, that means there is no net force acting on it but then how is it moving down if there is no force on it? No force means no acceleration but still it can have a constant velocity (no acceleration) with which it moves down. But why and how does it get that velocity?
 

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andyrk said:
Does tension at a point in a string try to pull the point in 2 directions?
Hold one end of a string in one hand. Apply a tension. How taut is the string? Hold one end of the same string in one hand, and the second end in the other and pull in opposite directions. How taut is the string? Can you apply tension by pulling on only one end?
andyrk said:
pulled up by a tension 2T?
The diagram shows two masses of 1 T hanging from the pulley by a string run over the pulley. Two times one is two.
andyrk said:
how is it moving down
It's not.
 
Bystander said:
Hold one end of a string in one hand. Apply a tension. How taut is the string? Hold one end of the same string in one hand, and the second end in the other and pull in opposite directions. How taut is the string? Can you apply tension by pulling on only one end?

The diagram shows two masses of 1 T hanging from the pulley by a string run over the pulley. Two times one is two.

It's not.
Right, for a string to have tension or remain taut, it needs to be connected or pulled from both ends with equal force.

But shouldn't it move down? Why should there be no forces on the unhinged pulley?
 
andyrk said:
Right, for a string to have tension or remain taut, it needs to be connected or pulled from both ends with equal force.

But shouldn't it move down? Why should there be no forces on the unhinged pulley?
Your second diagram lacks important information about masses and friction. Is there some accompanying text you've omitted?
 
andyrk said:
be no forces on the unhinged pulley?
Two T down, and two T up --- no indication in the diagram that the block anchoring the upper string is moving/sliding on the table top. The string supporting the lower pulley is NOT wrapped around the pulley, or turning it --- it's not shown specifically in the diagram, but in the real world, it would be attached to a clevis which carries the shaft around which the pulley turns.
 
haruspex said:
Your second diagram lacks important information about masses and friction. Is there some accompanying text you've omitted?
Nope. I just wanted to know that why is the unhinged pulley being pulled by a tension 2T upwards?
 
andyrk said:
Nope. I just wanted to know that why is the unhinged pulley being pulled by a tension 2T upwards?
how do you know that it is, other than that someone has drawn it on the diagram?
 
Because that's what the solution I am looking at says.

I didn't mention some facts which were also included in the question-
1.No frictional forces
2. Massless pulleys and strings

Does that somehow help you to give a reasoning as to why the pulley is being pulled up by tension 2T?
 
andyrk said:
Because that's what the solution I am looking at says.

I didn't mention some facts which were also included in the question-
1.No frictional forces
2. Massless pulleys and strings

Does that somehow help you to give a reasoning as to why the pulley is being pulled up by tension 2T?
That's why I asked about further information!
If an object is massless then it doesn't matter whether it is accelerating or not. ##\Sigma F = ma## tells you that the net force must be zero.
 
  • #10
Oops..sorry my bad. But how is it still moving down then?
 
  • #11
andyrk said:
Oops..sorry my bad. But how is it still moving down then?
I presume the three blocks have mass, so there should be the weights of the two smaller blocks acting down. It will turn out that these are less than 2T in sum, so those blocks will accelerate downwards. Since the strings do not break, they and the pulley must accelerate down too.
 
  • #12
The 2T up and the two Ts down cancel out. So by the virtue of which force does the pulley move down?
 
  • #13
andyrk said:
The 2T up and the two Ts down cancel out. So by the virtue of which force does the pulley move down?
Like I said, the pulley has no mass, so it needs no force to accelerate which ever way. Its motion is determined by whatever it is attached to.
To make it more realistic, you could let the pulley have a very small mass. When you work out the whole system you will now find that the tensions down slightly exceed the tension up, giving the pulley just the acceleration it needs to keep all the strings taut. The same applies to the strings themselves, etc.
The 'massless' fiction just means the mass is insignificant compared with the other masses in the system.
 
  • #14
What? Why? The tensions down always equal the tension up. How can they be slightly greater than the upper tension?
 
  • #15
andyrk said:
What? Why? The tensions down always equal the tension up. How can they be slightly greater than the upper tension?
Actually I got it backwards - forgot gravity. The tension up will exceed tension down.
The system is accelerating. If the pulley has mass then there must be a net force to accelerate it downwards. The acceleration will be less than g, so the net of the tensions must be upwards.
 
  • #16
So if the net of the tensions is upwards then would the pulley start moving upwards instead of downwards?
 
  • #17
andyrk said:
So if the net of the tensions is upwards then would the pulley start moving upwards instead of downwards?
No, you've forgotten gravity acting on the pulley (as I did). The net force on the pulley will be downwards, accelerating it down at the same rate as the rest of the system. But that rate is less than g, so the net force of the strings must be upwards.
 
  • #18
But for the pulley to move down, why does need to have greater upper tension than lower? Even if they are same, pulley can still move down because of its mass. So why do the upper and lower tensions need to be different?
 
  • #19
andyrk said:
for the pulley to move down, why does need to have greater upper tension than lower?
That's not what I said.
For the pulley to accelerate down, the net force must be downwards: tensions down + mg > tension up. But the system will accelerate at a rate less than g, and for that reason tensions down < tensions up.
 
  • #20
haruspex said:
That's not what I said.
For the pulley to accelerate down, the net force must be downwards: tensions down + mg > tension up. But the system will accelerate at a rate less than g, and for that reason tensions down < tensions up.
If tensions down = tensions up still, tensions down + mg > tension up. So why is tensions down < tensions up?
 
  • #21
andyrk said:
If tensions down = tensions up still, tensions down + mg > tension up. So why is tensions down < tensions up?
The downward acceleration will be < g, so the net downward force must be < mg. Tdown+mg-Tup < mg. Tdown<Tup .
 
  • #22
haruspex said:
The downward acceleration will be < g, so the net downward force must be < mg. Tdown+mg-Tup < mg. Tdown<Tup .
I didn't get the inequalities you just showed. Can you explain them once again?
Why should Tdown+mg-Tup be < mg? Is there any reason for it?
 
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  • #23
andyrk said:
I didn't get the inequalities you just showed. Can you explain them once again?
Why should Tdown+mg-Tup be < mg? Is there any reason for it?
Let the mass of the pulley be m and the acceleration of the system (i.e. all the bits that move) be a. Do you agree they will all have the same acceleration? Do you see why a < g?
For the pulley, Tdown+mg-Tup = ma < mg.
 
  • #24
If the two masses are moving down, then T < mg. Then, if the pulley is massless, the 2T = T + T. So, the 2T < 2mg.

Is this what you were saying, andyrk? If so, then I agree.

Chet
 
  • #25
haruspex said:
That's why I asked about further information!
If an object is massless then it doesn't matter whether it is accelerating or not. ##\Sigma F = ma## tells you that the net force must be zero.
But wait, why would the pulley be pulled by two forces T and T in the downward direction on either side of the pulley in the first place? Shouldn't the points at which the pulley is being pulled downwards by T also be pulled upwards by T (since tension at a point acts in two directions), such that effectively the pulley isn't being pulled down at all and so we don't need the 2T force to exist? But this is not the case as we see in the image in post #1. Can somebody explain this?
 
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  • #26
andyrk said:
But wait, why would the pulley be pulled by two forces T and T in the downward direction on either side of the pulley in the first place? Shouldn't the points at which the pulley is being pulled downwards by T also be pulled upwards by T (since tension at a point acts in two directions), such that effectively the pulley isn't being pulled down at all and so we don't need the 2T force to exist? But this is not the case as we see in the image in post #1. Can somebody explain this?
In reality, the rope exerts a radial force on the pulley at all points where it contacts the pulley. But that makes it rather complicated to analyse, so typically you treat the part of the rope in contact with the pulley as part of the pulley. Now it's easy, the straight part exerts a pull T on the end of the curved part.
 
  • #27
haruspex said:
In reality, the rope exerts a radial force on the pulley at all points where it contacts the pulley. But that makes it rather complicated to analyse, so typically you treat the part of the rope in contact with the pulley as part of the pulley. Now it's easy, the straight part exerts a pull T on the end of the curved part.
But that T is in two opposite directions right?
 
  • #28
andyrk said:
But that T is in two opposite directions right?
Yes, but that's normal action and reaction. The straight section of rope pulls on the curved part+pulley, while the curved part+pulley pulls on the straight section.
 
  • #29
haruspex said:
Yes, but that's normal action and reaction. The straight section of rope pulls on the curved part+pulley, while the curved part+pulley pulls on the straight section.
Oh. So the two T's don't act on the pulley itself? Only the upper one does? So why doesn't it happen the other way round? That is, why doesn't the curved part + pulley pull the straight part up and the straight part pulls the curved part + pulley down? So that the two T's instead of being down are up?
 
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  • #30
I see, the 2T tension in the upper string would also reverse its direction in that case. Either way, either the two tensions acting on the pulley are down or u but not both. Am I right? And the 2T tension above adjusts its direction accordingly. Right?
 
  • #31
andyrk said:
I see, the 2T tension in the upper string would also reverse its direction in that case. Either way, either the two tensions acting on the pulley are down or u but not both. Am I right? And the 2T tension above adjusts its direction accordingly. Right?
You are aware that when you have an action-reaction pair at the contact point between two bodies A and B, one member of the pair is the force exerted by body B on body A, and the other member of the pair is the force exerted by body A on body B, correct? When you are doing a force balance on body A, the two don't cancel. The force balance on body A includes only forces exerted by other bodies on body A, and not forces exerted by body A on other bodies. If both members of an action-reaction pair always had to be included, then no body could ever exert a force on any other body.

Can you see how this all relates to your rope and pulley?

Chet
 
  • #32
Chestermiller said:
You are aware that when you have an action-reaction pair at the contact point between two bodies A and B, one member of the pair is the force exerted by body B on body A, and the other member of the pair is the force exerted by body A on body B, correct? When you are doing a force balance on body A, the two don't cancel. The force balance on body A includes only forces exerted by other bodies on body A, and not forces exerted by body A on other bodies. If both members of an action-reaction pair always had to be included, then no body could ever exert a force on any other body.

Can you see how this all relates to your rope and pulley?

Chet
So is the action reaction logic the reason why a point in a rope has tensions in two opposite directions all throughout the rope? And if that is the case then why does the end of the string still have tension T while the block is pulling the string down with force m1g on one end and m2g on the other end?
 
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  • #33
andyrk said:
So is the action reaction logic the reason why a point in a rope has tensions in two opposite directions all throughout the rope?
Suppose you have a rope under tension T (with both of its ends fixed), and you decide to cut the rope at a certain location. Say the rope is horizontal, and, after you cut it, you have a left section and a right section. You decide what you are going to do is, by hand, replace the force that the right section was exerting on the left section, so that the tension within the left section is the same as it was before. What force would you have to apply by hand to accomplish this? What direction would this force be pointing?

Now you decide to do the same thing with the right section, rather than the left section. What force would you have to apply by hand to the right section so that it is under the same tension as before? What direction would this force be pointing?

Chet
 
  • #34
Chestermiller said:
Suppose you have a rope under tension T (with both of its ends fixed), and you decide to cut the rope at a certain location. Say the rope is horizontal, and, after you cut it, you have a left section and a right section. You decide what you are going to do is, by hand, replace the force that the right section was exerting on the left section, so that the tension within the left section is the same as it was before. What force would you have to apply by hand to accomplish this? What direction would this force be pointing?

Now you decide to do the same thing with the right section, rather than the left section. What force would you have to apply by hand to the right section so that it is under the same tension as before? What direction would this force be pointing?

Chet

For the left section, I would have to apply the same force that the right section was pulling it with when it was not cut. And for the right section, I would have to apply the same force that the left section was pulling it with when it was not cut. But whether the two forces are equal or not is still unclear.
 
  • #35
andyrk said:
For the left section, I would have to apply the same force that the right section was pulling it with when it was not cut. And for the right section, I would have to apply the same force that the left section was pulling it with when it was not cut. But whether the two forces are equal or not is still unclear.
If you go around to the other side of the string, the left side becomes the right side, and right side becomes the left side. So the forces have to be the same, since the place where you personally are located can't affect the string.

Chet
 
  • #36
Chestermiller said:
If you go around to the other side of the string, the left side becomes the right side, and right side becomes the left side. So the forces have to be the same, since the place where you personally are located can't affect the string.

Chet
What? What do you mean by left side becomes right side and vice-versa? I still don't get why the forces would have to be equal? Oh. Okay. I get it. But what about the ends of the string when it is connected to blocks at the two ends? If the block pulls the string down by a force equal to its weight then shouldn't the string pull it back with the same force leading to a tension at the ends which is equal to the weight of the block attached to the end of the string? But that is not the case as we know
 
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  • #37
andyrk said:
What? What do you mean by left side becomes right side and vice-versa? I still don't get why the forces would have to be equal? Oh. Okay. I get it. But what about the ends of the string when it is connected to blocks at the two ends? If the block pulls the string down by a force equal to its weight then shouldn't the string pull it back with the same force leading to a tension at the ends which is equal to the weight of the block attached to the end of the string? But that is not the case as we know
If the block is accelerating, then it does not pull the string down by a force equal to its weight. It pulls the string down by a force less than its weight:

Newton's 2nd law:

T - mg = -ma

If the block pulled the string down with a force equal to its weight, then it would be in equilibrium, and couldn't be accelerating.

Chet
 
  • #38
Right. How could I forget that.
 
  • #39
andyrk said:
Right. How could I forget that.
If it were me, I would blame it on a "Senior Moment." But you're much younger than I am.

Chet
 
  • #40
Chestermiller said:
If it were me, I would blame it on a "Senior Moment." But you're much younger than I am.

Chet
What's a senior moment? And what about the other end? Why does the tension at the other end also equal T? ( The block is accelerating upwards here). Why can't it be something other than T which would impart the same acceleration to the lighter block as the heavier block on the other end?
 
  • #41
andyrk said:
What's a senior moment?

A senior moment refers to what happens to your memory when you become a senior citizen.

And what about the other end? Why does the tension at the other end also equal T? ( The block is accelerating upwards here). Why can't it be something other than T which would impart the same acceleration to the lighter block as the heavier block on the other end?
This follows from a moment balance on the pulley. Unlike the blocks, the pulley is assumed to be massless, so that its moment of inertial is also zero. So, ##T_1R-T_2R=I\alpha = 0##, and thus T2 = T1.

Chet
 
  • #42
Chestermiller said:
A senior moment refers to what happens to your memory when you become a senior citizen.This follows from a moment balance on the pulley. Unlike the blocks, the pulley is assumed to be massless, so that its moment of inertial is also zero. So, ##T_1R-T_2R=I\alpha = 0##, and thus T2 = T1.

Chet
What? Wait, the tensions at the pulley can be equal but why do they also need to be equal at the ends connected to the 2 blocks?
 
  • #43
andyrk said:
What? Wait, the tensions at the pulley can be equal but why do they also need to be equal at the ends connected to the 2 blocks?
If you do a force balance on the section of a massless string between the pulley and a block, you get

$$T_{by \ pulley}-T_{by \ block}=(string \ section \ mass)\times (string \ section \ acceleration)=0$$

Chet
 
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  • #44
Chestermiller said:
If you do a force balance on the section of a massless string between the pulley and a block, you get

##T_{by \ pulley}-T_{by \ block}=(string \ section \ mass)\times(string \ section \ acceleration)=0##

Chet
So do you mean to say that the block is pulling the string at the end with a tension T and not its weight?
 
  • #45
andyrk said:
So do you mean to say that the block is pulling the string at the end with a tension T and not its weight?
Yes. I though we already settled that.

Chet
 
  • #46
Chestermiller said:
Yes. I though we already settled that.

Chet
Yup but I was thinking that what stops the string from having tension equal to the weight? Is Newton's Second Law a sufficient enough reason? That is, the block accelerates so their has to be a net force. Is that a good enough reason why T would not and should not equal the weight of the block?

Chestermiller said:
If you do a force balance on the section of a massless string between the pulley and a block, you get

##T_{by \ pulley}-T_{by \ block}=(string \ section \ mass)\times(string \ section \ acceleration)=0##

Chet
And we can calculate this unknown T by solving the equations we make with the help of Newton's Second Law, right?
 
  • #47
andyrk said:
Yup but I was thinking that what stops the string from having tension equal to the weight? Is Newton's Second Law a sufficient enough reason? That is, the block accelerates so their has to be a net force. Is that a good enough reason why T would not and should not equal the weight of the block?

Sure. We either accept Newton's 2nd law, or we don't. Personally, I accept it.
And we can calculate this unknown T by solving the equations we make with the help of Newton's Second Law, right?
Sure. That's what this is all about.

Chet
 
  • #48
Chestermiller said:
You are aware that when you have an action-reaction pair at the contact point between two bodies A and B, one member of the pair is the force exerted by body B on body A, and the other member of the pair is the force exerted by body A on body B, correct? When you are doing a force balance on body A, the two don't cancel. The force balance on body A includes only forces exerted by other bodies on body A, and not forces exerted by body A on other bodies. If both members of an action-reaction pair always had to be included, then no body could ever exert a force on any other body.

Can you see how this all relates to your rope and pulley?

Chet
One final question, why does the rope have to pull the pulley down at the point it touches the pulley and not up? Since tension can be in either direction, so why does it have to be down only?
 
  • #49
andyrk said:
One final question, why does the rope have to pull the pulley down at the point it touches the pulley and not up? Since tension can be in either direction, so why does it have to be down only?
If the string were exerting an upward force on the pulley, the string would have to be under compression. Have you ever seen what happens to a string when you try to put it under compression? But that still doesn't prevent you from drawing an upward arrow for the force of the string acting on the pulley at the contact point, and it doesn't prevent you from drawing a downward arrow for the force of the pulley on the string. However, when you solve the problem, the value of this force would come out negative, indicating that the arrows should be pointing in the opposite direction.

Chet
 
  • #50
Chestermiller said:
However, when you solve the problem, the value of this force would come out negative, indicating that the arrows should be pointing in the opposite direction.
You mean when I apply Newton's law on the blocks and strings and get the tension, I would get a specific direction for tension? But as I understood it, tension is always acting in 2 directions. So how can I get a single direction? Lastly, why doesn't the string have tension pointing in 2 directions at the point it is pulling the pulley down? (Even though it is unclear as to why it pulls it down..that is another question altogether at the moment).
 
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