A pulley system with two pulleys and two suspended masses

AI Thread Summary
The discussion revolves around a pulley system with two pulleys and two suspended masses, questioning the movement of blocks A and B based on their masses. The participants clarify that the solution assumes equal masses, which determines the direction of movement. They also explain that the relationship between the movements of the blocks is derived from the lengths of the rope segments, specifically that if block B moves up by 1 cm, block A moves down by 2 cm due to the configuration of the pulleys. The conversation further delves into the mathematical representation of the system, focusing on how to express the total length of the rope and the changes in variables as the blocks move. Overall, the thread emphasizes the importance of understanding the constraints and relationships in the system to solve the problem accurately.
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Homework Statement
Pls see below
Relevant Equations
Pls see below
For this problem,
1677189160333.png

The solution is,
1677189178930.png

However, how do they know the block B will move up and block A will move down? The masses of each are not given so could be the other way round if ##m_b > m_a##?

Also how do they know that if block B moves up by 1cm, block A will move down by 2cm?

Many thanks!
 
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The problem states that the masses are equal and the solution is based on that.
 
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kuruman said:
The problem states that the masses are equal and the solution is based on that.
Thank you for your reply @kuruman !

Sorry I did not see that! I will try the problem again.

Many thanks!
 
Callumnc1 said:
Also how do they know that if block B moves up by 1cm, block A will move down by 2cm?
That is a matter of 'counting': in the picture you see three lengths of cord. Think of the situation that block A is all the way down: by then A has dropped by two lengths, whereas B has gone up by only one length.

##\ ##
 
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BvU said:
That is a matter of 'counting': in the picture you see three lengths of cord. Think of the situation that block A is all the way down: by then A has dropped by two lengths, whereas B has gone up by only one length.

##\ ##
Thank you for your reply @BvU!

I think I might see what you mean from intuition, is there way to prove this thought?

Many thanks!
 
Callumnc1 said:
Thank you for your reply @BvU!

I think I might see what you mean from intuition, is there way to prove this thought?

Many thanks!
1677200458048.png


Write the total length of the inextensible rope ##L##, In terms of all the other lengths of each section. There will be a couple more steps, but that is where you start.
 

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Callumnc1 said:
is there way to prove this thought?

Yes ! The overwhelming beauty of physics: The experiment decides !

##\ ##
 
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erobz said:
View attachment 322795

Write the total length of the inextensible rope ##L##, In terms of all the other lengths of each section. There will be a couple more steps, but that is where you start.
Thank you for your reply @erobz ! That diagram is quite helpful :)

## L = l + s + 2.5 \times purple~semicircle##

Many thanks!
 
BvU said:
Yes ! The overwhelming beauty of physics: The experiment decides !

##\ ##
Thank you for your reply @BvU!
 
  • #10
Callumnc1 said:
Thank you for your reply @erobz ! That diagram is quite helpful :)

## L = l + s + 2.5 \times purple~semicircle##

Many thanks!
Sorry, I shouldn't have drawn that top section purple, it could be any length. I'll update the image.

1) just assign a random variable to each length that is not already labeled.
2) you are missing some length of rope in that sum.
 
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  • #11
erobz said:
Sorry, I shouldn't have drawn that top section purple, it could be any length.

1) just assign a random variable to each length that is not already labled
2) you are missing some length of rope in that sum.
Thank you for your reply @erobz !

Is the ok for the variables?
1677200509314.png

Many thanks!
 
  • #12
From the diagram it looks like ##c = b##, but would you like me to leave it like that @erobz ?

Many thanks!
 
  • #13
Callumnc1 said:
Thank you for your reply @erobz !

Is the ok for the variables?
View attachment 322798
Many thanks!
Yeah, that will work.
 
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  • #14
erobz said:
Yeah, that will work.
Thank you for your reply @erobz !

##L = a + s + b + c + l##

Many thanks!
 
  • #15
Callumnc1 said:
Thank you for your reply @erobz !

##L = a + s + b + c + l##

Many thanks!
ok, but you are still missing a length of rope there.
 
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  • #16
erobz said:
ok, but you are still missing a length of rope there.
Thank you for your reply @erobz !

Sorry should be ##L = a + 2s + b + c + l## and assuming that the pulleys are the same size as the rope is taut, then ##c = b ## so simplifying gives ##L = a + 2s + 2b + l##

Many thanks!
 
  • #17
Callumnc1 said:
Thank you for your reply @erobz !

Sorry should be ##L = a + 2s + b + c + l##

Many thanks!
Great! Now identify the only variables that change in that equation when the blocks move.
 
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  • #18
erobz said:
Great! Now identify the only variables that change in that equation when the blocks move.
Thank you for your reply @erobz !

The variables that change are ##l## and ##s##

Many thanks!
 
  • #19
Callumnc1 said:
Thank you for your reply @erobz !

The variables that change are ##l## and ##s##

Many thanks!
I guess they are functions of time then?

Many thanks!
 
  • #20
Callumnc1 said:
I guess they are functions of time then?

Many thanks!
Don't worry about that just yet.

So ##l## and ##s## are the only length that can change. Apply a change to each of the variables.

For instance if a varianle was ##z## we would apply a change by adding ##\Delta z## to it. etc...

Write the new equation.
 
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  • #21
erobz said:
Don't worry about that just yet.

So ##l## and ##s## are the only length that can change. Apply a change to each of the variables.

For instance if a varianle was ##z## we would apply a change by adding ##\Delta z## to it. etc...
Thank you for your reply @erobz !

The change for each length is

##\Delta l##
##\Delta s##

Which in the original equation is

##L = a + 2\Delta s + 2b + \Delta l##Many thanks!
 
  • #22
Callumnc1 said:
Thank you for your reply @erobz !

The change for each length is

##\Delta l##
##\Delta s##

Many thanks!
So what is the new equation? Rember a variable that changes goes from ##z \to z+ \Delta z##.
 
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  • #23
Thank you for your reply @erobz !

I this this equation,

##L = a + 2\Delta s + 2b + \Delta l##

Can also be expressed as##L_i = L_f##
## a + 2s_i + 2b + l_i = a + 2s_f + 2b + l_f##
## 2s_i + l_i =2s_f+ l_f##

Many thanks!
 
  • #24
erobz said:
So what is the new equation? Rember a variable that changes goes from ##z \to z+ \Delta z##.
Thank you for your reply @erobz!

Do you mean

##z_i = z_f + \Delta z##?

If you want I could edit post #23 to use that notation. This is giving me conservation of string vibes I remember sometime talking about it on Discord.

Many thanks!
 
  • #25
Callumnc1 said:
Thank you for your reply @erobz!

Do you mean

##z_i = z_f + \Delta z##?

If you want I could edit post #23 to use that notation. This is giving me conservation of string vibes I remember sometime talking about it on Discord.

Many thanks!
you don't need the subscripts. Its just saying you take what was labeled ##z## in the original eq. and replace it with ##z + \Delta z##.
 
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  • #26
I think @erobz that,

## L_i = 2s_i + l_i =2s_f+ l_f = L_f##

is really just a conservation of string statement, correct?

Many thanks!
 
  • #27
erobz said:
you don't need the subscripts. Its just saying you take what was labeled ##z## in the original eq. and replace it with ##z + \Delta z##.
Oh ok thank you for your reply @erobz !

I'm not too familiar with that notation. I will change to that notation.

Many thanks!
 
  • #28
Callumnc1 said:
Oh ok thank you for your reply @erobz !

I'm not too familiar with that notation. I will change to that notation.

Many thanks!
I believe it's the standard we approach stuff in Calculus.
 
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  • #29
Hi @erobz ,

Is the reason why you used arrows for this ##z \to z+ \Delta z## because if you use equal sign then

##z = z+ \Delta z##
##z = z+ z_f - z_i##
##z_i = z_f##

Oh which is conservation of the quantity z anyway!

Many thanks!
 
  • #30
erobz said:
I believe it's the standard we approach stuff in Calculus.
Oh thank you for your reply @erobz !
 
  • #31
Here it is @erobz ,

##L = a + 2s + \Delta 2s+ 2b + l + \Delta l##

Many thanks!
 
  • #32
Callumnc1 said:
Hi @erobz ,

Is the reason why you used arrows for this ##z \to z+ \Delta z## because if you use equal sign then

##z = z+ \Delta z##
##z = z+ z_f - z_i##
##z_i = z_f##

Oh which is conservation of the quantity z anyway!

Many thanks!
Its just shorthand math notation for saying ##z## goes to ## z + \Delta z##. The variable ##z## wouldn't equal ## z + \Delta z## except in the case that ##\Delta z \to 0##
 
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  • #33
erobz said:
Its just shorthand math notation for saying ##z## goes to ## z + \Delta z##. The variable ##z## wouldn't equal ## z + \Delta z## except in the case that ##\Delta z \to 0##
Thank you for your reply @erobz !

So an equivalent notation is

##z ≈ z + dz##
 
  • #34
Callumnc1 said:
Here it is @erobz ,

##L = a + 2s + \Delta 2s+ 2b + l + \Delta l##

Many thanks!
Ok, now equate the two equations through the variable ##L## and cancel the terms. What are you left with?

Edit: keep the ##\Delta## next to the ##s##
 
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  • #35
erobz said:
Ok, now equate the two equations through the variable ##L## and cancel the terms. What are you left with?
Thank you for your reply @erobz!

Which two equations sorry?

Many thanks!
 
  • #36
Callumnc1 said:
Which two equations sorry?

Many thanks!
The first one we derived with that one. they both equal ##L##. You are attempting to figure out how the changes in each variable relate to each other.
 
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  • #37
erobz said:
The first one we derived with that one. they both equal ##L##.
Thank you for your reply @erobz !

That must be ##L = a + 2s + 2b + l## and ##L = a + 2s + \Delta 2s+ 2b + l + \Delta l##

So
##a + 2s + 2b + l = a + 2s + \Delta 2s+ 2b + l + \Delta l##
## 0 = \Delta 2s + \Delta l##
## -\Delta 2s = \Delta l##
## 2(s_f - s_i) = l_f - l_i##
Many thanks!
 
  • #38
Callumnc1 said:
Thank you for your reply @erobz !

That must be ##L = a + 2s + 2b + l## and ##L = a + 2s + \Delta 2s+ 2b + l + \Delta l##

So
##a + 2s + 2b + l = a + 2s + \Delta 2s+ 2b + l + \Delta l##
## 0 = \Delta 2s + \Delta l##

Many thanks!
Move one of them to the other side of the zero. And if you want to know how far pulley B moves in terms of a how far pulley A moves solve for ##\Delta s##.
 
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  • #39
Again. Keep the ##\Delta## touching the ##s##. They are stuck together. Joined at the hip! don't put that 2 in between them.
 
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  • #40
erobz said:
Again. Keep the ##\Delta## touching the ##s##. They are stuck together. Joined at the hip! don't put that 2 in between them.
Thank you for your reply!

Sorry @erobz missed that message,

## -2\Delta s = \Delta l##

Many thanks!
 
  • #41
Thank you for your help @erobz !

Just a side question, how were we allowed to add the ##\Delta## to ##s## and ##l## then set them equal to each other?

Many thanks!
 
  • #42
Callumnc1 said:
Thank you for your help @erobz !

Just a side question, how were we allowed to add the ##\Delta## to ##s## and ##l## then set them equal to each other?

Many thanks!
Because the change is unsigned. It could be a positive change. It could be a negative change. It may appear like were adding to both lengths but is turns out we weren't. Notice the equation dictates a positive change in the variable ##l## ( ##\Delta l > 0##) demands and negative change in ##s## ( ##\Delta s < 0 ##), and visa-versa.
 
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  • #43
erobz said:
Because the change is unsigned. It could be a positive change. It could be a negative change. It may appear like were adding to both lengths but is turns out we weren't. Notice the equation dictates a positive change in the variable ##l## ( ##\Delta l > 0##) demands and negative change in ##s## ( ##\Delta s < 0 ##), and visa-versa.
Thank you for your reply @erobz !

I think we can only add the ##\Delta## to the variable that is changing if know that there is a constraint for example the string length is conserved, correct?

Many thanks!
 
  • #44
Callumnc1 said:
Thank you for your reply @erobz !

I think we can only add the ##\Delta## to the variable that is changing if know that there is a constraint for example the string length is conserved, correct?

Many thanks!
No. You can add it to anything. The only constraint needed is that you have a relationship between some variables. It's simply saying we have this relationship between all these variables, lets pick some or, all that can change and change them a bit from where they currently are valued at, and see how they respond to each other. How it all pans out or the end goal is specific to each situation.

The main motivation is derivatives and differential equations, where you are looking for the change in one variable w.r.t a change in another variable. You've got time to learn all this. You don't have to figure all this out yesterday.
 
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  • #45
erobz said:
No. You can add it to anything. The only constraint needed is that you have a relationship between some variables. It's simply saying we have this relationship between all these variables, lets pick some or, all that can change and change them a bit from where they currently are valued at, and see how they respond to each other. How it all pans out or the end goal is specific to each situation.

The main motivation is derivatives and differential equations, where you are looking for the change in one variable w.r.t a change in another variable. You've got time to learn all this. You don't have to figure all this out yesterday.
Thank you for your help @erobz ! :)
 
  • #46
Callumnc1 said:
##L = a + 2\Delta s + 2b + \Delta l##
No, the deltas are the increases in length. The original lengths should still be in the equation. You should have just replaced ##s## with ##s+\Delta s##, etc.
 
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  • #47
I am somewhat flabbergasted at the length (:wink:) of this thread!
If you do the experiment with a real piece of rope things will be clear quickly.

If you still insist on a mental exercise, remove all unessentials: reduce the pulleys to points, etc

##\ ##
 
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  • #48
haruspex said:
No, the deltas are the increases in length. The original lengths should still be in the equation. You should have just replaced ##s## with ##s+\Delta s##, etc.
o_O It was getting late! I guess my mind was just inserting symbols that weren’t there.

Edit: Actually at a later post (#31) than what you must have been quoting they did get the proper result.
 
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  • #50
haruspex said:
No, the deltas are the increases in length. The original lengths should still be in the equation. You should have just replaced ##s## with ##s+\Delta s##, etc.
Thank you for your reply @haruspex ! I will try that sometime.

Many thanks!
 

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