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A pulley system with two pulleys and two suspended masses
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SUMMARY
The forum discussion centers on the mechanics of a pulley system involving two pulleys and two suspended masses. The participants clarify that the solution assumes equal masses for blocks A and B, which dictates their movement: if block B moves up by 1 cm, block A moves down by 2 cm due to the configuration of the rope. The total length of the inextensible rope is expressed as L = a + 2s + 2b + l, where variables represent different lengths in the system.
PREREQUISITES- Understanding of basic physics principles, specifically mechanics.
- Familiarity with pulley systems and their configurations.
- Knowledge of algebraic manipulation of equations.
- Concept of conservation of string in mechanical systems.
- Study the principles of mechanical advantage in pulley systems.
- Learn about the conservation of energy and its application in pulley problems.
- Explore the derivation of equations of motion for systems involving pulleys.
- Investigate the role of tension in ropes and its effects on motion in pulley systems.
Students of physics, mechanical engineers, and anyone interested in understanding the dynamics of pulley systems and their applications in real-world scenarios.
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erobz
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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##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!
member 731016
Thank you for your reply @erobz !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##
So an equivalent notation is
##z ≈ z + dz##
erobz
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Ok, now equate the two equations through the variable ##L## and cancel the terms. What are you left with?Callumnc1 said:
Edit: keep the ##\Delta## next to the ##s##
member 731016
Thank you for your reply @erobz!erobz said:Ok, now equate the two equations through the variable ##L## and cancel the terms. What are you left with?
Which two equations sorry?
Many thanks!
erobz
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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.Callumnc1 said:Which two equations sorry?
Many thanks!
member 731016
Thank you for your reply @erobz !erobz said:The first one we derived with that one. they both equal ##L##.
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!
erobz
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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##.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!
erobz
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Again. Keep the ##\Delta## touching the ##s##. They are stuck together. Joined at the hip! don't put that 2 in between them.
member 731016
Thank you for your reply!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.
Sorry @erobz missed that message,
## -2\Delta s = \Delta l##
Many thanks!
member 731016
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!
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!
erobz
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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.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!
member 731016
Thank you for your reply @erobz !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.
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!
erobz
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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.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!
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.
Last edited:
member 731016
Thank you for your help @erobz ! :)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.
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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.Callumnc1 said:##L = a + 2\Delta s + 2b + \Delta l##
BvU
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I am somewhat flabbergasted at the length (
) 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
##\ ##
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
##\ ##
erobz
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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.
Edit: Actually at a later post (#31) than what you must have been quoting they did get the proper result.
Last edited:
Lnewqban
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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/
member 731016
Thank you for your reply @haruspex ! I will try that sometime.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.
Many thanks!
member 731016
Thank you for your reply @BvU!BvU said:I am somewhat flabbergasted at the length () 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
##\ ##
Sorry, what do you mean reduce the pulley to points?
Many thanks!
member 731016
Thank you for your reply @erobz !erobz said: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.
member 731016
Thank you for sharing that thread @Lnewqban !Lnewqban said: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/
View attachment 322810
View attachment 322811
BvU
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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 ..
##\ ##
member 731016
Ok thank you @BvU !BvU said:You can get far with just a few pins or paperclips and a piece of wire, real or imagined ..
##\ ##
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