Inclined Pulley system, little information given.

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Homework Help Overview

The discussion revolves around an inclined pulley system problem where the original poster is attempting to derive an expression for velocity in terms of length, angle, and gravitational acceleration. The problem involves analyzing the forces and tensions in the system, with limited information provided regarding the masses involved.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster discusses the assumption that tensions in the rope are equal and that the velocities of the masses are the same. They express a need for an expression for velocity and question how to eliminate mass variables from their equations. Other participants engage by suggesting a ratio of masses and exploring the implications of assuming equal masses.

Discussion Status

Participants are exploring various assumptions and interpretations of the problem, particularly regarding the masses involved. Some guidance has been offered regarding the relationship between the variables, but there is no consensus on how to proceed due to the lack of specific mass information.

Contextual Notes

The original poster notes that they are not given any information about the masses or their ratios, which complicates their ability to solve the problem. There is a suggestion that the problem may have been poorly stated, leading to uncertainty about the assumptions that can be made.

alexgmcm
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Homework Statement


I have dutifully reproduced the problem in OODraw please forgive the poor aesthetic quality but I believe all the important information is visible.
fnYb6.jpg

Homework Equations


[tex]mgL-Lsin(\theta)m'g = \frac{mv^2}{2} + \frac{m'v'^2}{2}[/tex]
[tex]T=T'[/tex]
[tex]v=v'[/tex]
[tex]\therefore v^2 = \frac{2gl(m-m'sin(\theta)}{m+m'}[/tex]
[tex]v = \sqrt{\frac{2gl(m-m'sin(\theta)}{m+m'}}[/tex]

Also:

[tex]m'a = T-m'gsin(\theta)[/tex]
[tex]ma = mg - T[/tex]
[tex]\therefore m(g-a)=m'(a+gsin(\theta))[/tex]

The Attempt at a Solution



I assumed that T must be equal to T' as it is the same rope and hence can only have one tension? It just seemed to make more sense. The Lsin(theta) bit comes from the assumption that the rope length remains constant and hence m' is dragged parallel to the slope the same distance that m falls. I also assumed that v' must equal v as otherwise the rope would break, I just don't see how it could make physical sense if they weren't equal.

I need an expression for V in terms of L and theta and possibly g. That makes the second part of the question solvable. But I cannot see how to cancel the expressions for the masses out of my equations.

Any help?
 
Last edited:
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You're right, there is no way to cancel m or m', because the speed depends on them.

The best you can do is set [tex]M = m/m'[/tex] to get

[tex]v = \sqrt{\frac {2 g l (M - sin(\theta))} {M+1} }[/tex]
 
Hmmm.. that doesn't help with the second part of the question though where i have to show that it is equal to 1.5ms^-1 for certain parameters, because I am not given any info about the masses or their ratios.

I wonder if we are meant to assume m=m' and the question has just been given poorly. I will see what I can get with that assumption.
 
Putting m=m' we get that:
[tex]v= \sqrt{gL(1-sin(\theta))}[/tex]

However for L=1, theta = 20 degrees, this yields a value of 2.54ms^-1 not 1.5ms^-1 as specified in the question.

Therefore m cannot equal m'.

Unfortunately given the fact that I have no information about the masses I cannot see a solution to this problem!?
 

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