High School What is the Correct Reading on the Scale in This Mass/Scale Puzzle?

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The discussion revolves around understanding the tension in a cable system with a scale and weights. Participants debate the reading of the scale when a 10kg weight is involved, with one asserting that the scale should read 10kg, while others question why it wouldn't read 20kg given the apparent forces. The key point emphasized is that tension in a rope under equilibrium conditions is uniform and does not double, as it must balance the forces acting on it. Various scenarios are proposed to clarify this concept, but the consensus remains that the scale measures the tension accurately as 10kg. The conversation highlights the nuances of tension and force in physics, illustrating common misconceptions.
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TL;DR
What does the scale read in this diagram?
My learning is a bit rusty. I can intuit the answer but I can't formalize it.


What does the scale read?
1753225663323.webp



I say the scale reads 10kg.

My logic is this:
  1. Fix the left cable and pulley in place with a giant glob of glue.
  2. Cut the cable holding the left weight.
  3. The scale is holding up a 10kg weight. Nothing has changed as far as the scale is concerned.

But what is a more elegant way of getting the answer?
 
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That's fine, but also: The rope can only have one tension. It can't be 10kg by each weight and 20 in the middle (a common error).
 
DaveC426913 said:
TL;DR Summary: What does the scale read in this diagram?

  1. Fix the left pulley in place with a big glob of glue.
  2. Cut the cable holding the left weight.
  3. The scale is holding up a 10kg weight. Nothing has changed as far as the scale is concerned.
I think you meant to describe it in a different way. If you fix the left pulley and cut the cable at the left weight, the left cable fragment slips over the fixed pulley and the scale is pulled over the right pulley by the right weight. Fixing the left pulley does not constrain the left cable (modulo the low friction between the left cable and the left fixed pulley).

I think you meant something more like "attach the left cable to a wall instead of the pulley and weight... :smile:
 
berkeman said:
I think you meant to describe it in a different way. If you fix the left pulley and cut the cable at the left weight, the left cable fragment slips over the fixed pulley and the scale is pulled over the right pulley by the right weight.
Sorry, you're right, what I wrote was ambiguous.

I meant a giant glob of glue that affixes both pulley and cable in place.
 
russ_watters said:
That's fine, but also: The rope can only have one tension. It can't be 10kg by each weight and 20 in the middle (a common error).
I don't follow. Who says it would be 10kg by each weight?
 
DaveC426913 said:
I don't follow. Who says it would be 10kg by each weight?
Since the weight is stationary (i.e., not accelerating), the tension pulling up on the weight must exactly balance the gravitational force pulling down on it.
 
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DaveC426913 said:
I don't follow. Who says it would be 10kg by each weight?
Suppose you eliminate the pulley on the left and tie the cable to a fixed block resting on the table top, as shown in the figure below. What will the scale read?
1753239619047.webp


Next, hang the scale and a 10 kg block from the ceiling, as shown in the figure below. What will the scale read?
1753239763208.webp


Hopefully, you can see that in all cases the tension in the cable is the same.
 
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DaveC426913 said:
I don't follow. Who says it would be 10kg by each weight?
I mean the weight is 10kg, so where the cable attaches to the weight the upward force on the weight is 10kg.
 
renormalize said:
Since the weight is stationary (i.e., not accelerating), the tension pulling up on the weight must exactly balance the gravitational force pulling down on it.
Just to note that is the definition of tension. It's the force transmitted; not twice the force transmitted!
 
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  • #10
Mister T said:
Suppose you eliminate the pulley on the left and tie the cable to a fixed block resting on the table top, as shown in the figure below. What will the scale read?
View attachment 363602

Next, hang the scale and a 10 kg block from the ceiling, as shown in the figure below. What will the scale read?
View attachment 363603

Hopefully, you can see that in all cases the tension in the cable is the same.
Yes. That was exactly my logic in the opening post. (Ijust glued the left pulley and cable solid.)

What I'm not grasping is Russ' alternate explanation in post 2.
 
  • #11
DaveC426913 said:
Yes. That was exactly my logic in the opening post. (Ijust glued the left pulley and cable solid.)

What I'm not grasping is Russ' alternate explanation in post 2.
Newton's laws demand that a rope in equilibrium can only have one tension throughout. Unless it has intermediate contact points.

There's no logic as such. The definition of tension is the force. Not twice the force transmitted.
 
  • #12
DaveC426913 said:
What I'm not grasping is Russ' alternate explanation in post 2.
I don't see it as an alternate explanation.

Once you go through the sequence of scenarios associated with each situation shown in the figures, you conclude that the tension is the same in all three scenarios. It's therefore an error to think the tension doubles in the first scenario. In all cases you are attaching the ends of a cable to a scale in a place where you could have just tied the two ends together instead. In other words, cut a cable anywhere and insert a scale between the cut ends, the scale by definition measures the tension in the cable.
 
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  • #13
Mister T said:
I don't see it as an alternate explanation.

Once you go through the sequence of scenarios associated with each situation shown in the figures, you conclude that the tension is the same in all three scenarios. It's therefore an error to think the tension doubles in the first scenario.
Right. That's the same as my opening analysis. But it's not elegant because it requires saying "OK, let's look at this alternate layout and now you can see it's the same as the given layout." I would be that is not how it is solved in physics classes.

I have to assume there's more direct explanation, one that simply analyzes the given diagram irecxtly.


Mister T said:
In all cases you are attaching the ends of a cable to a scale in a place where you could have just tied the two ends together instead. In other words, cut a cable anywhere and insert a scale between the cut ends, the scale by definition measures the tension in the cable.
I'm not sure that helps me.

I see what you're saying:
1753281251180.webp

I just don't follow why it's still only 10kg except by using the "look at this alternate scenario" method.
 
  • #14
Let me rephrase:

Can you show - formally, and without using an alternate scenario for contrast - why the scale shows only 10kg, when it appears to the naive eye, to be under 20 kg of tension.
1753281362038.webp
 
  • #15
DaveC426913 said:
Let me rephrase:

Can you show - formally, and without using an alternate scenario for contrast - why the scale shows only 10kg, when it appears to the naive eye, to be under 20 kg of tension.
View attachment 363617
If the spring is stretched to the point where it shows ##10g## on the display, then it provides a ##10g## force at either end. That's how its calibrated. You could calibrate it so that it shows ##20g## at that point. But, all you've done is redefined the measure of tension.

You can't prove a definition.
 
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  • #16
DaveC426913 said:
Right. That's the same as my opening analysis. But it's not elegant because it requires saying "OK, let's look at this alternate layout and now you can see it's the same as the given layout." I would be that is not how it is solved in physics classes. I'm not sure that helps me.
It appears in Paul G. Hewitt's famous "Next Time Questions". In the instructor's guide, which accompanies his Conceptual Physics textbook, that is the way he explains the answer.

DaveC426913 said:
I have to assume there's more direct explanation, one that simply analyzes the given diagram irecxtly.
If you pull on a cable with a force of magnitude ##F## the cable pulls back on you with a force of magnitude ##F##. You can measure this magnitude by inserting a scale between you and the cable. Orient it so that it reads the force exerted by you. Flip it around so that it reads the force exerted by the cable. In both cases the scale reads ##F##, verifying the validity of Newton's Third Law. The value of ##F## is by definition the tension in the cable.

DaveC426913 said:
I see what you're saying:
View attachment 363616
I just don't follow why it's still only 10kg except by using the "look at this alternate scenario" method.
It's not the only method. It's just a heuristic method used to help clarify or reinforce. Replacing the 10 kg block hanging on the left with the fixed block attached to the table top shows that they both perform the same function. They each exert the same magnitude force on the cable, therefore the hanging block doesn't add anything to the magnitude of the force exerted on the scale.
 
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  • #17
Are you guys pulling my leg? How is that not 20kg in tension?
 
  • #18
Bandersnatch said:
Are you guys pulling my leg? How is that not 20kg in tension?
You could define it as 20kg if you want, but then the force would be given by ##F = T/2##.
 
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  • #19
Bandersnatch said:
Are you guys pulling my leg? How is that not 20kg in tension?
So the [not fully baked] idea is that you sum the magnitude of the force exerted out the one way and the magnitude of the force exerted out the other way? These forces being exerted by a slice of negligible thickness?

That idea is not ideal since tension can be a signed quantity. A negative tension is a pressure. For example in a stiff rod.

One can generalize the notions of tension and pressure and shear forces with the Cauchy Stress Tensor. By convention (or, equivalently, by definition), the components of that tensor are not doubled. Now instead of looking at magnitudes, one is looking at force per unit area (tensor) multiplied by an incremental directed area (vector) yielding an incremental force (vector). And the signs come out perfectly.
 
  • #20
PeroK said:
If the spring is stretched to the point where it shows ##10g## on the display, then it provides a ##10g## force at either end. That's how its calibrated. You could calibrate it so that it shows ##20g## at that point. But, all you've done is redefined the measure of tension.

You can't prove a definition.
But ... there's 20kg pulling on it!
 
  • #21
DaveC426913 said:
But ... there's 20kg pulling on it!
Define it as 20kg then! It won't change the physics. As above, you'll just need to use ##F = T/2## in your free-body diagrams.
 
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  • #22
DaveC426913 said:
But ... there's 20kg pulling on it!
But forces are vectors. That's -100 N on the left and +100 N on the right for a total of 0 N. No surprise there. The rope is not accelerating.

Which is, I guess, the central point. Just because you can add two numbers together does not mean that you should.

[Yes, I know that you are only trying to help pull our collective legs!]
 
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  • #23
Bandersnatch said:
Are you guys pulling my leg? How is that not 20kg in tension?
I know, right?


I mean, I am satisfied that it is 10kg, but only because of the way I went about it:
1753292181158.webp

It obviously shows 10kg in diagram 2. And diagram 1 is the sam, as far as the scale goes so it must also be 10kg.

I just think that's a pretty sloppy way to demonstrating it.
 
  • #24
jbriggs444 said:
But forces are vectors. That's -200 N on the left and +200 N on the right for a total of 0 N. No surprise there. The rope is not accelerating.
OK. I see that explains why it's not moving, but that still doesn't really explain why it's 10 and not 20.

jbriggs444 said:
Which is, I guess, the central point. Just because you can add two numbers together does not mean that you should.
Well, if I added 10 kg to each side, that would certainly add to the tension put on the cable. So it makes sense that I should be adding the weights up.

jbriggs444 said:
[Yes, I know that you are only trying to help pull our collective legs!]
I'm really not.

It's a conundrum.

I know the correct answer. I even have my own way to demonstrate it intuitively.
But I also know it's not the way they would teach the solution to it in a physics class.
 
  • #25
DaveC426913 said:
OK. I see that explains why it's not moving, but that still doesn't really explain why it's 10 and not 20.
Use the Newton meter in its usual configuration hanging from a ceiling, hang a 10kg mass from it and let it settle. In that configuration it has a 100N force pulling it down from the mass. It must also have a 100N force pulling it up from the ceiling attachment, otherwise it would be accelerating by Newton's second law. You want this to read 100N.

In the horizontal case in the OP you have 100N forces on each end, just as in the experiment I described above. So it should read 100N (or 10kg depending how it's calibrated).
 
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  • #26
Bandersnatch said:
Are you guys pulling my leg? How is that not 20kg in tension?
Did you not read Post #7?
 
  • #27
Ibix said:
In the horizontal case in the OP you have 100N forces on each end, just as in the experiment I described above. So it should read 100N (or 10kg depending how it's calibrated).
Or, 200N if you want to calibrate it that way!
 
  • #28
DaveC426913 said:
But ... there's 20kg pulling on it!
Is that not also true of the two alternate scenarios I described in Post #7? Do you honestly believe that when you hang 3 lb of bananas from a spring scale the scale will read 6 lb? Remember you have 3 lb of force pulling down on the scale and 3 lb of force pulling up on the scale. The scale is in a state of static equilibrium, the net force on it is zero.
 
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  • #29
Mister T said:
Is that not also true of the two alternate scenarios I described in Post #7? Do you honestly believe that when you hang 3 lb of bananas from a spring scale the scale will read 6 lb?
No, it would read 6lb if I had 3lb of bananas hanging off one side and 3lb off the other side.
 
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  • #30
I get that, if you hung a 10kg mass from the ceiling, there is 10kg pulling down and 10 kg pulling up.

I think that's the crux. All the pulleys do is change one of them from 'up' to 'down'. No, that would cancel to zero. :sorry:

Is there a FBD diagram that would demonstrate the solution?

Maybe show why I think there's a missing 10kg? Will it show 5kg pulling on each end of the scale?

How would you solve this problem - with formulae, say, on an test?
 
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