Lagrange equations of motion for hoop rolling down moving ramp.

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Homework Help Overview

The discussion revolves around deriving the Lagrange equations of motion for a hoop rolling down an inclined plane that is capable of sliding on a horizontal surface. The problem involves concepts from classical mechanics, particularly Lagrangian mechanics, and the dynamics of rolling motion.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the breakdown of kinetic energy into components and the choice of generalized coordinates. There is an exploration of constraints related to rolling without slipping and the relationship between different axes of motion.

Discussion Status

Some participants have provided guidance on selecting appropriate coordinates and expressing kinetic and potential energy in terms of those coordinates. There is ongoing exploration of the implications of the ramp's movement on the system's dynamics.

Contextual Notes

Participants note confusion regarding the integration of different motion components and the representation of variables, particularly with respect to the movement of the ramp and the hoop's rolling motion.

Strukus
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Homework Statement


A hoop of mass m and radius R rolls without slipping down an inclined plane of mass M, which makes an angle [tex]\alpha[/tex] with the horizontal. Find the Lagrange equations and the integrals of the motion if the plane can slide without friction along a horizontal surface.

Homework Equations


L = T - U

T = kinetic energy
U = potential energy

Inertia tensor of hoop = mr[tex]^{2}[/tex]

The Attempt at a Solution


Here's what I believe to be the situation.
homework3-1.jpg


I know that I have to break up the kinetic energy into its separate components, but I'm not entirely sure how. I have 2 examples to work with, one being a block sliding down a moving ramp and the other being a hoop rolling down a stationary ramp.

Here's the block.

homework3-1b.jpg


Here's the hoop.
homework3-1a.jpg


With the block, we break it down into velocity along the x-axis and the y-axis for both the block and the ramp (with the ramp's y-velocity being 0). But with the hoop, we break up the velocity into an x'-axis (axis at the same angle as the ramp) and a [tex]\theta[/tex]. Both of the examples make sense to me, though combining them in this way leaves me a little confused.

If I were to just solve with what I knew now, I would combine the rotational velocity, the velocity along the x-axis, and the velocity along the y-axis into the kinetic energy.
 
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When you do Lagrangian problems, a good starting point is to decide on your generalized coordinates and then write any constraints relating them. So what are your generalized coordinates and what are your constraints?
 
I'm going to use the hoop on the non-moving ramp as my reference for this.

It has the equation of constraint being what describes the rolling without slipping, so
f = dx' - r d[tex]\theta[/tex] = 0
f = [tex]\dot{x}[/tex]' - r [tex]\dot{\theta}[/tex] = 0

And y-ramp = 0.

And the generalized coordinates are x' and [tex]\theta[/tex].

That makes sense to me, but since the ramp is moving I'll have to describe the x-axis movement in terms of the x'-axis movement or describe the x'-axis movement in terms of the x-axis and y-axis, which is where I'm getting stuck.

And I'm not sure why but whenever I preview the post it's not what I typed (in terms of the greek letters).
 
It is better to use x for the horizontal position of the ramp (more conventional) and s for the coordinate down the plane, relative to the plane. Keep angle θ as you have it. Can you write expressions for the kinetic energy T and the potential energy U in terms of these coordinates?
 
Last edited:
Wow, that really helps. I forget what example it was when I was taking notes in class but I forgot with this approach you can kind of just use whichever axes you wish and it will still work.

That being said, this is what I have come up with.

T = 1/2 M [tex]\dot{x}[/tex][tex]^{2}[/tex] + 1/2 m [tex]\dot{s}[/tex][tex]^{2}[/tex] + 1/2 m r[tex]^{2}[/tex] [tex]\dot{\theta}[/tex][tex]^{2}[/tex]
U = m g s sin[tex]\alpha[/tex]
 
Last edited:
After much working it through, looking at sample problems, and asking for help, I finished it! Thank you for your help kuruman!
 
I hope you wrote the translational kinetic energy of the center of mass of the rolling hoop correctly. It is not simply

[tex]\frac{1}{2}m\dot{s}^2[/tex]

It is

[tex]\frac{1}{2}m(\dot{s}cos\alpha+\dot{x})^2+\frac{1}{2}m(\dot{s}sin\alpha)^2[/tex]

:wink:
 
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