Rolling and Friction: Explaining the Paradox

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Discussion Overview

The discussion revolves around the mechanics of a wheel being pulled by a string, focusing on the role of friction in enabling rolling motion versus sliding. Participants explore the conditions under which friction is considered or ignored in calculations of torque and motion.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant notes that friction is necessary for the wheel to roll without slipping, yet questions why it can be ignored in certain calculations.
  • Another participant suggests that friction is often neglected to simplify the analysis, but acknowledges its critical role in preventing sliding.
  • A different viewpoint emphasizes that static friction does not do work and thus can be excluded from motion equations, but is essential for initiating rotation.
  • One participant calculates the friction force needed for rolling, indicating that it is a significant factor in the overall force required to pull the wheel.
  • Another participant compares scenarios where the wheel is lifted versus resting on the ground, questioning the differences in frictional effects in both cases.
  • There is a suggestion to consider different models of the wheel (e.g., as a cylinder or a ring) to analyze how this affects the required frictional force.

Areas of Agreement / Disagreement

Participants generally agree that friction is necessary for rolling, but there is no consensus on how to treat it in calculations or the implications of ignoring it. Multiple competing views on the role and treatment of friction remain present in the discussion.

Contextual Notes

Some participants express uncertainty regarding the assumptions made about the wheel's motion and the conditions under which friction can be neglected. The discussion also reflects varying interpretations of the physical models applied to the wheel.

Chen
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Suppose there's a wheel on the ground, radius R, and I'm pulling it with a string connected the top of the wheel with force T.

We know that if we want the wheel to roll, there has to be friction between the ground and the wheel. But at the same time we ignore that friction and say that the only force on the wheel is T, and the torque is:
N = RxT

So why do we require the existence of friction but also sort of ignore it? I know that it's correct I just want to understand why.

Thanks. :smile:
 
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I'm not quite sure how you want the string to be attached, but to answer your question, we ignore friction so that you can neglect any minor losses which are due to it, but you need to know it does exist otherwise the wheel might slide before it rolls, and this isn't how you want to approach your problem.
 
here is the answer

you should appraoch the problem like this:
if friction is not there your sphere will slide because there is no force to ratate it about the centroidal axis.
here the friction that comes into effect is static friction which by it's defination does not do any work. That is the reason why we do not take friction into account while solving the motion's eqation.
 
The friction acts on the wheel to start it turning. You can calculate the force of friction from the acceleration of the axis and the moment of inertia of the wheel. This will definitely be a contribution to the force you called T. If you are pulling a wheel by a string, the force needed to start the wheel spinning is 1/3 the total force. This is the friction force and it definitely is not ignorable. In a sense, the static friction sets up the proportion of energy that ends up in rotational (Iomega^2/2) vs. translational (mv^2/2) (v here is the velocity of the c.of m.).

OTOH, if you are pulling a large vehicle where the mass is much larger than the mass of the wheels, you can often safely ignore this effect.
 
krab already answered, but I'll add my two cents.

Chen said:
We know that if we want the wheel to roll, there has to be friction between the ground and the wheel. But at the same time we ignore that friction and say that the only force on the wheel is T, and the torque is:
N = RxT
Cleary if a frictional force exists, you can't ignore it! The torque would not be RxT!

krab figured out the frictional force needed to have the wheel roll without slipping (F = T/3). In doing so, he treated the wheel as a cylinder or disk ([itex]I = 1/2mR^2[/itex]).

Just for fun, figure out the frictional force needed if you model the wheel as a ring ([itex]I = mR^2[/itex]).
 
If one lifts the wheel off the ground and then pulls the top part of the wheel
with a force T, it'll certainly rotate.
So how is this situation different from the wheel being on the ground+friction absent?



spacetime
www.geocities.com/physics_all/
 
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spacetime said:
If one lifts the wheel off the ground and then pulls the top part of the wheel
with a force T, it'll certainly rotate.
So how is this situation different from the wheel being on the ground+friction absent?
It's not different. If a friction force exists, it contributes to the net torque about the center of mass. The static friction simply prevents slipping between the wheel and the ground.
 

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