[High school physics] Wheel touching a kerb. What are the forces on the wheel?

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Homework Help Overview

The discussion revolves around the forces acting on a wheel that is about to lift over a kerb of height h. The original poster presents a scenario involving the application of a force at the axle and the weight of the wheel, while also considering the role of friction and normal forces at the point of contact.

Discussion Character

  • Conceptual clarification, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants explore the forces acting on the wheel, including tangential friction, horizontal force, weight, and normal reaction force. There is a debate about the necessity of friction for the wheel to lift over the kerb and the implications of different force diagrams.

Discussion Status

Some participants have provided insights into the mechanics of the situation, discussing the importance of pivoting about the contact point and the relationship between the weight of the wheel and the forces involved. There is ongoing questioning regarding the presence of friction and its role in the lifting process, with no clear consensus reached.

Contextual Notes

Participants are grappling with the implications of friction and normal forces in a theoretical context, with references to specific scenarios such as an ice kerb. The discussion includes considerations of infinitesimal geometry and the physical behavior of materials at the point of contact.

Nanyang
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[Solved] Wheel touching a kerb just about to lift. What are the forces on the wheel?

Homework Statement


In order to lift a wheel over a kerb of height h, a minimum force F is be applied at the axle. The radius of the wheel is R. Draw all the forces on the wheel then find its weight.

*IMAGE003*

Homework Equations


T = r X F

The Attempt at a Solution


I managed to find the weight of the wheel. But what I am confused about is the drawing of the forces on the wheel.

My teacher presented a drawing like this below.

f is the tangential friction on the wheel.
F is the horizontal force at the axle.
W is the weight of the wheel.
N is the normal reaction force at the point of contact.

*IMAGE003a*

Since he argued that without friction the wheel will slide and therefore the wheel cannot be pushed up the kerb. Thus we must conclude that the normal reaction force on the point of contact is not passing through the center of the wheel, otherwise that point will move.

However I do not understand. Because if we imagine the surface of the point of contact is an infinitesimally flat surface, and the friction is parallel to the surface but the normal reaction force would be perpendicular to the surface. Therefore N would pass through the center for geometrical reasons.

However this is a dilemma. Since if there is friction then that point of contact will move. So I must conclude that there is no friction present. In other words, since there is no force parallel to that surface in contact, there cannot be any static friction.

So instead my drawing is like below.
*IMAGE003b*

Which is correct? My teacher gave an example of the situation on an ice kerb. He says that it will otherwise be impossible for the wheel to be lifted up by the horizontal force. However, I feel that even if there is no friction it is possible for the wheel to be lifted up the kerb.

Both drawings give the same answer to the weight of the wheel since it is done by taking the torque relative to the point of contact.
 

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I realized my drawings are too large! Sorry for that! :)
 
For the wheel to lift itself over the curb, it must pivot about the contact point. And friction must prevent slip (no slip implies static friction).

Applying the weight of the wheel at is center of mass, then what is the moment arm between the CM and contact point? One must consider the angle between the moment arm and weight.
 
Yes I have found the weight to be

W = F [(R -h) / (h(2R - h))^0.5]

But I still cannot understand why is there friction...
 
Nanyang said:
However I do not understand. Because if we imagine the surface of the point of contact is an infinitesimally flat surface, and the friction is parallel to the surface but the normal reaction force would be perpendicular to the surface. Therefore N would pass through the center for geometrical reasons.
Reasoning with infinitessimals is tricky -- you should put little faith in such arguments unless you really know what you're doing, or you know how to turn the argument into a sound one without infinitessimals.

e.g. once we start thinking about very, very small scales, we have to worry about the wheel and curb deforming at the point of contact to accommodate the forces involved. And even an "infinitessimal" change in an "infinitessimal" surface can have a large effect on the direction of the normal.
 

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