What is the acceleration of a point on the circumference of the disk?

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Homework Help Overview

The discussion revolves around determining the acceleration of a point on the circumference of a disk that is influenced by a hanging mass. The problem involves concepts from rotational dynamics and forces acting on both the disk and the hanging mass.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to relate the forces acting on the disk and the hanging mass using torque and moment of inertia equations. Some participants question the assumption that the force exerted on the disk is simply the weight of the hanging mass, suggesting that string tension must also be considered. Others propose drawing free-body diagrams to clarify the forces at play.

Discussion Status

Participants are actively engaging with the problem, exploring different interpretations of the forces involved. Some guidance has been offered regarding the importance of string tension and the need for free-body diagrams to derive the necessary equations. The original poster has acknowledged a misunderstanding and has provided a revised expression for acceleration based on the discussion.

Contextual Notes

There is mention of a massless string and the lack of information regarding certain parameters, which may affect the analysis. The original poster's initial approach appears to overlook the role of tension in the system.

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Homework Statement



http://urlcut.com/katrolafbeelding.gif

What is the accelaration of a point on the circumference of the disk?

Homework Equations



[tex]\tau[/tex] = F.R = I.[tex]\alpha[/tex]

I = M.R²/2

a = R.[tex]\alpha[/tex]

F(z) = m.g

The Attempt at a Solution



The mass exerts a force F(z) = m.g on the disk. This force is what puts the disk into motion with [tex]\tau[/tex] = F(z).R = m.g.R (1)

Also, as I = M.R²/2 and a = R.[tex]\alpha[/tex] and [tex]\tau[/tex] = I.[tex]\alpha[/tex]
==> [tex]\tau[/tex] = M.R.a/2 (2)

Out of (1) & (2):

m.g.R = M.R.a/2 <=> m.g = M.a/2 <=> a = 2m.g/M

The acceleration asked for is a = 2m.g/M

But the teacher's solution says: [tex]\frac{2m.g}{2m+M}[/tex]

What have I done wrong?
 

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I can't view your problem or picture yet, but if this is a disk being accelerated by a hanging mass, the force exerted on the disk is not mg. The mass and disk are connected by a string, and it's the string tension which accelerates the disk. The string's tension and the weight cannot be the same, or else the hanging object would be at rest.
 
You can't view the picture? What does it say when you click it. (EDIT: made visible)

Also, it said that the rope was without mass. I'm not really familiar with string tension. There is no information given about the string tension coëfficient (if something like that exists, at least), its length, girth, etc... I don't see how it fits in.
 
Last edited:
Draw a free-body diagram of the hanging mass. There are two forces acting on it. This will give you an expression for a in terms of tension T and other constants. Same goes for a torque expression for the disk. 2 equations with 2 unknowns.

I can't see the picture yet because it must be approved by the forum moderators first.
 
Oh I see... So the string tension is somewhat like the normal force of suspended objects. (probably a bad analogy, but yeah...)

So the force acting on the disk is not the gravitational force nor the string tension, but the difference between the two. So:

m.g - L = m.a <=> L = m.g - m.a = m(g-a) (1)

And we also had the equation [tex]\tau[/tex] = L.R = I.[tex]\alpha[/tex]
and we get (after substitution using the other equations):

L = M.a/2 (2)

Out of (1) & (2):

m(g-a) = M.a/2 <=> m.g - m.a = M.a/2 <=> 2m.g = M.a + 2m.a <=> a = [tex]\frac{2m.g}{2m+M}[/tex]

THANKS!
 

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