Tension in pulley systems Concept help

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Discussion Overview

The discussion revolves around understanding the concept of tension in pulley systems, particularly in the context of Newton's laws of motion. Participants explore the relationships between forces acting on masses connected by a pulley, including how to derive equations for tension and acceleration.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant seeks clarification on the equation T - mg = ma, expressing confusion about how tension is derived in the context of two masses on a pulley.
  • Another participant suggests that the lecturer may have oversimplified the explanation, prompting a discussion about the relationship between the accelerations of the two masses.
  • It is proposed that while the blocks may have different accelerations, they are constrained by the taut rope, leading to a specific relationship between their accelerations.
  • A participant emphasizes the importance of drawing free-body diagrams and applying Newton's laws to derive the necessary equations for the system.
  • There is a clarification that the accelerations of the two blocks are not necessarily the same, but they are related due to the kinematic constraint of the rope's length.
  • One participant acknowledges a previous misunderstanding regarding the necessity of having three equations to solve for the unknowns in the problem.

Areas of Agreement / Disagreement

Participants express differing views on whether the accelerations of the two masses must be the same. While some argue they can differ, others initially suggested they might be equal under certain conditions. The discussion remains unresolved regarding the implications of these differing perspectives.

Contextual Notes

Participants note the importance of kinematic constraints in the problem, highlighting that the length of the rope affects the relationship between the masses' accelerations. There is also mention of needing multiple equations to solve for the unknowns, indicating potential gaps in understanding the problem setup.

Who May Find This Useful

This discussion may be useful for students studying mechanics, particularly those grappling with concepts related to tension in pulley systems and the application of Newton's laws.

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I need help understanding why in problems tension is modeled as T-mg = ma.

I understand there are different variations, but the main concept is what I need help with.

For example:

If i have 2 masses hanging off a pulley (m1=5kg & m2=10kg) then m1 has a downward force of 49N down. The formula given is T-m1g=ma. and i understand that t-m1a=g is the force, which is why it is set = to ma, BUT i cannot grasp the concept of how tension is found that way and why for m2 it is m2g-T2=m2a..

I need a good concrete explanation. Baby steps and spell it out for me to understand please!
 
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Okay:
I think,perhaps, your lecturer is a bit too swift on this, and has made some simplifications that can seem rather confusing.

We'll start with the following observation:
The rope is taut, and of the same length all the time (agreed to that one?).
Now, try to formulate, in your own words:
If we call object 1's acceleration a_1, object 2's acceleration a_2, what must be the relation between these two accelerations?
 
arildno said:
Okay:
I think,perhaps, your lecturer is a bit too swift on this, and has made some simplifications that can seem rather confusing.

We'll start with the following observation:
The rope is taut, and of the same length all the time (agreed to that one?).
Now, try to formulate, in your own words:
If we call object 1's acceleration a_1, object 2's acceleration a_2, what must be the relation between these two accelerations?

considering its in a system where a is constant wouldn't the acceleration be the same?
 
The blocks will have different accelerations. You apply Newton's 2d Law for each block. It's possible they will be the same, but not necessary.

I would suggest you start attacking the problem by drawing free-body diagrams of each blocks. Then define your coordinate system/reference frame(s), get the kinematics of the block (this is very simple for rectilinear motion!), and apply Newton's 2d Law.

You will get your "formula" from the free-body diagrams.
 
"wouldn't the acceleration be the same?"

They are equally "large", right, but while one block accelerates upwards, the other accelerates downwards. Agreed?

This gives us the equation I'll call (1):

a_1=-a_2 (1) (Here, the minus sign is included to indicate acceleration in opposit directions!)

"considering its in a system where a is constant "
Do you understand that this is irrelevant?

The crucial factor is that IF block 1 didn't accelerate upwards as much as block 2 accelerates downwards (or vice versa), THEN the distance between them, measured as the length of the rope, would change. It does not matter whether the acceleration is constant or not. Do you understand that?

-----------------------------------------
" It's possible they will be the same, but not necessary."
Completely incorrect. That the rope is taut and remains of the same length throughout the period, is a kinematic constraint on the problem at hand; as necessary to handle as everything else. You have three basic unknowns in your problem, hence you need three equations, not just two, in order to solve it.
Think about it..:smile:
 
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arildno said:
" It's possible they will be the same, but not necessary."
Completely incorrect. That the rope is taut and remains of the same length throughout the period, is a kinematic constraint on the problem at hand; as necessary to handle as everything else. You have three basic unknowns in your problem, hence you need three equations, not just two, in order to solve it.
Think about it..:smile:

I know; I'm not sure why I wrote what I did last night, but under the assumptions that were made that statement is indeed a falsehood.

Thanks for pointing that out.
 

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