A pulley system with two pulleys and two suspended masses

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Homework Help Overview

The discussion revolves around a pulley system involving two pulleys and two suspended masses. Participants explore the mechanics of the system, particularly the movement of the blocks and the relationship between the lengths of the rope sections.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants question how the direction of movement for blocks A and B is determined without given masses. They also inquire about the relationship between the distances moved by the blocks and the lengths of the rope.

Discussion Status

Some participants have provided insights into the mechanics of the system, suggesting that the movement of the blocks can be understood through the configuration of the rope. Others are exploring the implications of their assumptions and seeking further clarification on the relationships between the variables involved.

Contextual Notes

There are discussions about the equality of the masses and the implications of that assumption on the movement of the blocks. Participants also mention the need for clarity on the lengths of the rope sections and how they relate to the overall system dynamics.

  • #31
Here it is @erobz ,

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

Many thanks!
 
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  • #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!
 
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  • #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!
 
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  • #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 ! :)
 
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  • #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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  • #49
Callumnc1 said:
However, how do they know the block B will move up and block A will move down?
...
Also how do they know that if block B moves up by 1cm, block A will move down by 2cm?

Do you now understand how do they know those things?

If not, please see:
https://www.physicsforums.com/threa...2-dynamics-problem-involving-a-pulley.991370/

pully4a-gif.gif


support-25281-2529-gif.gif
 
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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!
 
  • #51
BvU said:
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

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

Sorry, what do you mean reduce the pulley to points?

Many thanks!
 
  • #52
erobz said:
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.
Thank you for your reply @erobz !
 
  • #54
Callumnc1 said:
Sorry, what do you mean reduce the pulley to points?

You can get far with just a few pins or paperclips and a piece of wire, real or imagined ..

##\ ##
 
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  • #55
BvU said:
You can get far with just a few pins or paperclips and a piece of wire, real or imagined ..

##\ ##
Ok thank you @BvU !
 

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