Speed of Cylinder & Hoop Down Ramp: Analysis

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Homework Help Overview

The discussion revolves around the analysis of the speed of a cylinder and a hoop as they roll down a ramp inclined at an angle theta. The problem involves concepts from dynamics and energy conservation, particularly focusing on the translational and rotational motion of the objects.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of conservation of energy, questioning whether the objects are allowed to roll and how that affects the kinetic energy terms involved. There is also an exploration of the relationship between potential energy and kinetic energy for rolling objects.

Discussion Status

Some participants have provided guidance on using conservation of energy to relate potential and kinetic energies. There is an ongoing exploration of the implications of different moments of inertia for the cylinder and hoop, with no explicit consensus reached yet.

Contextual Notes

The original poster expresses uncertainty about how to begin the problem and has not provided their initial attempts, which is a requirement for further assistance in this forum. The discussion includes considerations of the ramp's length and angle, as well as the specific characteristics of the objects involved.

missnuss
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Homework Statement



Consider both a cylinder of radius Rc and mass mc and a hoop of radius Rh and mass mh. If both are at the top of a ramp of length L and at an angle theta what are the objects speed at the bottom of the ramp?

Homework Equations





The Attempt at a Solution

 
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You have to show your work before people help you. That IS the modus operandi of this
forum. Check thread started by me for example...
 
Last edited:
Sorry. I didn't post what I had tried to do because I have no clue where to even start. I'm not looking for the answer, I just wanted some help.
 
Use conservation of energy. Are the cylinders "allowed" to roll down the ramp? If so, you have to add in a rotational kinetic energy term into your equation.
 
If L is the length of the ramp, then the bottom point of any symmetric object would be
at height [itex]L\sin \theta[/itex]. Using conservation of energy, the potential energy
at the top should be equal to the sum of translational and rotational kinetic energies
at the bottom. For an object with moment of inertia about its center of mass I,

[tex]mg(L \sin \theta)= \frac{1}{2}mv^2 + \frac{1}{2}I \omega^2[/tex]

for pure rolling motion, [itex]\omega = v/R[/itex] so

[tex]mg(L \sin \theta)= \frac{1}{2}mv^2 + \frac{1}{2}I \frac{v^2}{R^2}[/tex]

solving for v, we have

[tex]v = \left[\frac{2gL \sin \theta}{1+(I/mR^2)}\right]^{1/2}[/tex]

from here, you can derive special cases for different bodies, in your case, a solid
cylinder (or is it hollow) and a hoop.
 
Thank you so very much
 

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