Two cylinders rolling without slipping

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SUMMARY

The discussion centers on the dynamics of two cylinders rolling down ramps without slipping, specifically comparing cylinder A, which rolls directly on the ramp, and cylinder B, which hangs from smaller cylindrical bits. Both cylinders have identical masses and moments of inertia. The conclusion drawn is that both cylinders reach the bottom simultaneously due to equal friction forces and normal forces acting on them, despite the differences in their radii affecting their angular velocities. The torque generated by friction is consistent for both cylinders, leading to the same translational kinetic energy at the bottom of the ramp.

PREREQUISITES
  • Understanding of rotational dynamics, specifically torque and angular acceleration.
  • Familiarity with the concepts of potential energy and kinetic energy in mechanical systems.
  • Knowledge of the principle of rolling without slipping.
  • Basic grasp of moment of inertia and its impact on rotational motion.
NEXT STEPS
  • Study the equations of motion for rolling objects, focusing on torque and angular momentum.
  • Explore the relationship between linear velocity and angular velocity in rolling motion.
  • Investigate the effects of friction on rolling motion and energy conservation.
  • Learn about the impact of varying moments of inertia on the dynamics of different shapes in motion.
USEFUL FOR

This discussion is beneficial for physics students, educators, and anyone interested in understanding the principles of rotational dynamics and energy conservation in mechanical systems.

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Homework Statement


Two cylinders (radius R) start from rest and roll without slipping down ramps. They both have the same masses and moments of inertia. The ramps are both at the same angle. One cylinder (A) is directly on the ramp. The other (B) is hanging from two smaller cylindrical bits (radius r) which stick out from either side and are in contact with the ramp. Which reaches the bottom first?

Homework Equations



τ = I α
τ = F r
mgh
1/2 mv^2
1/2 Iω^2

The Attempt at a Solution



I used torque to figure out which would have the greater ω. The force providing torque is friction, which must be the same for each cylinder (same mass, same normal force). The difference is in r; so the cylinder with the smaller r-value must have the smaller torque and thus the smaller ω at any moment in time. I.e.:

τ = F_f r = I α = I Δω/Δt
ω(t) = (F_f t / I) r

So it would seem that cylinder B, with the smaller r, must also have a smaller ω.

I know that the following is true for both cylinders:
mgh = 1/2 mv^2 + 1/2 Iω^2

So it would seem that cylinder B must have a greater v, because it has a smaller ω.

But I'm confused for a few reasons:
1. For rolling without slipping, v_cm = r ω. So if ω is smaller, so is v. This (obviously) contradicts the conclusion that smaller ω means greater v.
2. If friction is providing torque, it is increasing the rotational kinetic energy of the cylinders. Does that then mean that it is doing work? That would make the energy equation above incorrect (since it assumes zero work is done).
3. When I imagine the problem in my head, cylinder B seems like it should spin faster than cylinder A.

Any insight into this question is very much appreciated!
 
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Mmm... do the cilindrical bits have mass? If they don't, then they would not affect the moment of inertia... If you have some diagram or picture you can upload, if would greatly help in understanding the problem :)
 
I don't have a scanner, so I had to make the image myself:

Wx4Ym.png

In case that doesn't work: http://imgur.com/Wx4Ym

The mass of the extra bits on cylinder B can be ignored because both objects have the same total mass and same moment of inertia...
 
If both cilinders have the same normal force (which is evenly distributed in the bits), then the friction force is the same, and they come to the floor at the same time. Cilinder B could be lower than A, but I think we can ignore this.
 
Thanks, but the prof who asked this question claimed that one of them reached the ground first. Unfortunately I can't remember which and am unable to ask him right now.

They both start with the same potential energy, but once they're rolling, one of them spins faster and so has less translational kinetic energy. Just can't decide which.
 
But, if the inner surfaces that are in contact to the two sides (bases) of the cilinder are not frictionless, there would be a reduction of the torque... And they would also reduce kinetic energy...
Anyway, all seems to indicate that they come at the same time.
 
But, if the inner surfaces that are in contact to the two sides (bases) of the cilinder are not frictionless, there would be a reduction of the torque... And it would also reduce kinetic energy...
Anyway, ignoring that, all seems to indicate that they come at the same time.
 
What indicates that they arrive at the same time? I don't follow your reasoning. You said it's because the friction forces are the same? They are, I think, but they must also provide different torques if they're applied at different distances from the axis of rotation...
 
I got it. The difference in the radius of cilinder A and the radius of the bits of cilinder B should account for the difference in angular speed...
 
  • #10
Exactly. (And yes, you can ignore friction between the sides of cylinder B and the inside of the track.)

Any ideas on how to proceed?
 
  • #11
Can you put what you have together with moment of force? That'll help you know which one reaches first.
 
  • #12
Yes, friction forces are applied at different distances from the axis. That said, the torque is greater for cilinder A, and it comes first.
One question: is the lower part of cilinder B contributing to normal force? If it isn't, the problem is now solved.
 
  • #13
I'm guessing it doesn't contribute to anything because B is spinning on an axe Δ which is it itself.
 

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