Conservation of mechanical energy

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Homework Help Overview

The discussion revolves around the application of conservation of mechanical energy to derive the velocity of a hanging mass attached to a cylinder. The original poster attempts to derive the equation v = √((2gh)/(1+.5(m/M)(r/R)^2)) based on the energy principles involved in the system, which includes a hanging mass, a cylinder, and a wheel.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the definitions of variables involved (m, M, r, R, h) and question the setup of the problem. There are discussions about the initial conditions of the small cylinder and its relationship to the hanging mass. Some participants suggest checking the usage of variables and the assumptions regarding the mass of the cylinder and the nature of the wheel.

Discussion Status

Participants are actively questioning the assumptions made in the original post and clarifying the relationships between the components of the system. There is a recognition of potential confusion regarding the definitions of variables and the moment of inertia of the wheel. Some guidance has been offered regarding the setup and the need for clarity in the problem statement.

Contextual Notes

There is a suggestion that the cylinder is considered massless, and participants are exploring the implications of this assumption on the moment of inertia calculations. The discussion also highlights potential discrepancies in the definitions of the variables used in the equation to be derived.

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Derive equation v= √((2gh)/(1+.5(m/M)(r/R)^2)) by applying conservation of mechanical energy.

A string is attached to a hanging mass and wrapped around a small cylinder. The hanging mass is released from rest from an initial height (h) and accelerates to the floor. The theoretical velocity (v) of the hanging mass just before it strikes the floor can be determined by applying conservation of mechanical energy to the system.

v =velocity
m =hanging mass
M =mass of wheel
r =radius of wheel
R =radius of small cylinder
h =height

Ei=Ef
KEi+PEi = KEf+PEf
mgh = .5mv^2 + .5Iw^2
mgh = .5mv^2 + .5(.5Mr^2)(v/R)^2
2mgh = mv^2 + (M/2)(r^2/R^2)v^2
2mgh = (m + (M/2)(r^2/R^2)) v^2
√((2mgh)/(m + (M/2)(r^2/R^2))) = vWhat am I doing wrong?
 
Last edited:
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Hello,

Firstly, please describe the problem in more detail. What do m, M, r, R and h stand for? In which situation you apply the conservation of mechanical energy?

1) You can divide both the numerator and the denominator (of the square root) by m.

2) Check if m and M are used correctly (seems like M is m and m is M).
 
DoItForYourself said:
Hello,

Firstly, please describe the problem in more detail. What do m, M, r, R and h stand for? In which situation you apply the conservation of mechanical energy?

1) You can divide both the numerator and the denominator (of the square root) by m.

2) Check if m and M are used correctly (seems like M is m and m is M).
I updated the post with more info but I think it's irrelevant.
The conservation of mechanical energy is KEi+PEi=KEf+PEf
KEi and PEf both equal 0
So I'm starting with the equation PEi = KEf or mgh = .5mv^2 + .5Iw^2

And I need to show work to rearrange it to v= √((2gh)/(1+.5(m/M)(r/R)^2))

I made a lower case m & r, and a capital M & R to show that they are different variables as I cannot to subscript on my computer.
 
Nice, this makes more sense. But I still have some questions:

1) Is the small cylinder initially in the same level with the hanging mass (h)?
2) The problem does not refer to a wheel. Is the wheel attached to the small cylinder? Or the wheel is the small cylinder?

I think that a sketch would help in this situation.
 
DoItForYourself said:
Is the small cylinder initially in the same level with the hanging mass (h)?
I cannot see that that matters. The mass descends by h, the wheel and cylinder do not.
DoItForYourself said:
The problem does not refer to a wheel. Is the wheel attached to the small cylinder? Or the wheel is the small cylinder?
I deduce that the cylinder is considered massless but is attached coaxially to a wheel.
Two things strike me as wrong, though.
1. The wheel is not described as a uniform disc, so I would have thought the moment of inertia was more like that of a ring, Mr2 (or MR2 - see 2 below).
2. Someone is confused between r and R. I suspect that these have been crossed over in the definitions. As it stands, the equation to be proved is wrong, and the attempt by anon is right (except for point 1).
 
haruspex said:
I cannot see that that matters. The mass descends by h, the wheel and cylinder do not.

I deduce that the cylinder is considered massless but is attached coaxially to a wheel.
Two things strike me as wrong, though.
1. The wheel is not described as a uniform disc, so I would have thought the moment of inertia was more like that of a ring, Mr2 (or MR2 - see 2 below).
2. Someone is confused between r and R. I suspect that these have been crossed over in the definitions. As it stands, the equation to be proved is wrong, and the attempt by anon is right (except for point 1).

Yes, this is absolutely right. The potential energy of wheel and cylinder will not be changed anyway.

I agree with the assumption that the small cylinder is massless.

1) If the wheel is a ring, does it have to be uniform in order for the moment of inertia to be Μr2?

2) If the wheel is a uniform disc, the equation to be proved is wrong only in terms of m and M (the ratio must be M/m). Right?
 
DoItForYourself said:
Nice, this makes more sense. But I still have some questions:

1) Is the small cylinder initially in the same level with the hanging mass (h)?
2) The problem does not refer to a wheel. Is the wheel attached to the small cylinder? Or the wheel is the small cylinder?

I think that a sketch would help in this situation.
Here's a diagram
20171117_090652.jpg
 

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Figured it out , thanks for taking your time to help me!

20171117_093821.jpg
 

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DoItForYourself said:
Yes, this is absolutely right. The potential energy of wheel and cylinder will not be changed anyway.

I agree with the assumption that the small cylinder is massless.

1) If the wheel is a ring, does it have to be uniform in order for the moment of inertia to be Μr2?

2) If the wheel is a uniform disc, the equation to be proved is wrong only in terms of m and M (the ratio must be M/m). Right?
Yes.
 

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