Mechanics: Cylinder rolling up a step without slipping

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Homework Help Overview

The problem involves a uniform cylinder rolling without slipping along a horizontal surface and encountering a step of height b. The goal is to determine the conditions under which the cylinder can continue rolling past the step and maintain positive kinetic energy.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the relationship between kinetic energy and potential energy, exploring how to express these in terms of the given variables. There are attempts to derive conditions for the initial speed u based on energy conservation principles.

Discussion Status

Some participants have made progress in formulating expressions for kinetic and potential energy. There is ongoing exploration of how to relate angular velocity to linear velocity, with guidance provided to express angular velocity in terms of the known quantities. Multiple interpretations of the problem are being considered, particularly regarding the variables involved.

Contextual Notes

Participants note the importance of ensuring that the correct variables are used, specifically distinguishing between u and v, and there is acknowledgment of potential errors in earlier calculations.

iopmar06
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Homework Statement



A uniform cylinder of radius R, length L and density \delta is rolling without slipping along a horizontal surface with constant centre of mass speed u at A. It then meets a step of height b. We wish to find the conditions under which the cylinder is able to continue past the step and roll along the surface B.

Untitled.jpg


Assuming no energy is lost due to friction or drag, the change in the total kinetic energy before and after must be equal and opposite to the change in gravitational potential energy. Find a requirement on the initial speed u such that the cylinder passes B with positive kinetic energy.


Homework Equations



As the disc is rolling without slipping it is possible to use v = \omegaR.

The total kinetic energy is given by

\frac{1}{2}I\omega^2 + \frac{1}{2}mx^2

where

I = \frac{1}{2}MR^2

and gravitational potential is given by mgh.

The Attempt at a Solution



You are told in the question that \Delta K = -\Delta P

The change in kinetic energy will be negative and thus the change in potential will be positive. I want the final kinetic energy to be positive thus

K > |\Delta K|.

That's about as far as I have gotten. Any tips on how to get started will be greatly appreciated.

Also, I'm not sure if \alpha is significant or not (the \alpha on the diagram, not the angular acceleration).

NB: Sorry about my equations, I'm still trying to get used to using LaTeX.
 
Last edited:
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Welcome to PF iopmar06,

Thanks for taking the time to properly layout your question.

iopmar06 said:
The total kinetic energy is given by

\frac{1}{2}I\omega^2 + \frac{1}{2}mx^2

where

I = \frac{1}{2}MR^2
Good. Now using these equations can you explicitly write an expression for the total kinetic energy of the cylinder before the step, using the information given in the question?

Can you also write an expression for the change in potential energy of the cylinder, again using the variables you are given in the question?
 
I think I may have worked it out.

Kinetic Energy is given by:

K = \frac{1}{2} I \omega^2 + \frac{1}{2} m v^2<br /> <br /> = \frac{1}{2} (\frac{1}{2} m R^2) \omega^2 + \frac{1}{2} mv^2

Then:

\Delta P = mg \Delta h = mga


\Delta K = - \Delta P = -mga

We want the kinetic energy of the cylinder rolling along B to be positive so

\frac{1}{4} mr^2 \omega^2 + \frac{1}{2}mv^2 -mga &gt; 0


\frac{1}{2} mv^2 &gt; mga - \frac{1}{4} mr^2 \omega^2


v^2 &gt; 2ga - \frac{(r \omega)^2}{2}
 
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So then the condition on the initial velocity is:

v &gt; \sqrt{2ga - \frac{(r \omega)^2}{2}}
 
iopmar06 said:
I think I may have worked it out.

Kinetic Energy is given by:

K = \frac{1}{2} I \omega^2 + \frac{1}{2} m v^2<br /> <br /> = \frac{1}{2} (\frac{1}{2} m R^2) \omega^2 + \frac{1}{2} mv^2

Then:

\Delta P = mg \Delta h = mga\Delta K = - \Delta P = -mga

We want the kinetic energy of the cylinder rolling along B to be positive so

\frac{1}{4} mr^2 \omega^2 + \frac{1}{2}mv^2 -mga &gt; 0\frac{1}{2} mv^2 &gt; mga - \frac{1}{4} mr^2 \omega^2v^2 &gt; 2ga - \frac{(r \omega)^2}{2}
Looks good so far :approve:. However, you are not given \omega explicitly. Therefore, you need to express the angular velocity in terms of the quantities that you are given (HINT: There are still a few pieces of information you haven't used, but you only need one of them).
 
Last edited:
That completely slipped my mind, thanks for pointing it out.

The cylinder is not slipping so

v = \omega r

Substituting this into the inequality gives

v^2 &gt; 2ga - \frac{1}{2} (r \frac{v}{r})^2

v^2 &gt; \frac{4ga}{3}

so

v &gt; 2 \sqrt{ \frac{ga}{3}}
 
iopmar06 said:
That completely slipped my mind, thanks for pointing it out.

The cylinder is not slipping so

v = \omega r

Substituting this into the inequality gives

v^2 &gt; 2ga - \frac{1}{2} (r \frac{v}{r})^2

v^2 &gt; \frac{4ga}{3}

so

v &gt; 2 \sqrt{ \frac{ga}{3}}
Not a problem. Looks good to me :approve:. However, as a minor point don't forget that you are asked to find a condition for u and not v.
 
Last edited:
Yeah I'm just in the habit of using v for velocity.

Anyway, thanks a lot for all your help.
 
iopmar06 said:
Anyway, thanks a lot for all your help.
A pleasure.
 
  • #10
The "a" in my answer should be a "b". I didn't look at the diagram properly.
 

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