Reaction force acting at the wheels of cars when turning

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Homework Help Overview

The discussion revolves around the forces acting on the wheels of cars when turning, specifically focusing on the reaction forces and normal forces involved. The subject area includes concepts from dynamics and friction in the context of circular motion.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the application of Newton's equations to the wheels as separate bodies and discuss the implications of maximum friction force versus acting friction force. Questions arise regarding the interpretation of normal forces and the dimensions of angular velocity terms.

Discussion Status

The discussion is ongoing, with participants providing interpretations and clarifications about the forces at play. Some guidance is offered regarding the need for a clear understanding of normal forces and the context of the problem, while multiple interpretations of the question are being explored.

Contextual Notes

There is a noted lack of sufficient information to compute numeric answers, and participants emphasize that the problem does not require such answers. The ambiguity in the definition of normal forces is also highlighted.

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Homework Statement
Suppose a car describing a circular trajectory of radius ##R##. Consider just a right and left wheel of the car, and suppose that the distance between the two of them is ##d##. What's the normal force acting on each of the wheels?

Then answer: these reactions are greater or weaker than the reactions of a static car
Relevant Equations
##F=ma##
Well, I considered the two wheels as two different bodies and I wrote Newton's equations for both of them
I considered the wheel closer to the centre of the circle, we have:
##\mu N_1 =mR\dot (\theta)##
So we can find ##N_1##

Doing the same thing, we can find ##N_2##
##\mu N_2 =m(R+d) \dot(\theta)##

Then, the more velocity, the more normal needed for the friction. So when it's static the normal are smaller.
 
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##\mu N## is the maximum friction force. Does not have to be the acting friction force.
 
BvU said:
##\mu N## is the maximum friction force. Does not have to be the acting friction force.
So what would it be the right way of calculating it?
 
It is not entirely clear, but I think the question is asking about forces on the wheels as bodies separate from the car and axles connecting them.
If so, "normal force" means the net normal force on a wheel, i.e. that component of the net force on the wheel which is parallel to the wheel's axis.
For this purpose, you do not need to separate out frictional force (which may anyway have a component in another direction).

Btw, what do you mean by ##R\dot(\theta)##? If you mean ##R\dot\theta##, what dimension should that have?
 
My interpretation of the question is that it is suggesting that you think about what prevents the car from tipping over.

You are not given enough information to compute a numeric answer. But you are not asked for a numeric answer.
 
jbriggs444 said:
My interpretation of the question is that it is suggesting that you think about what prevents the car from tipping over.

You are not given enough information to compute a numeric answer. But you are not asked for a numeric answer.
Yes, you are right - it is about the forces normal to the ground, i.e. vertical. In this context, merely specifying normal is ambiguous.
 
Like Tony Stark said:
So what would it be the right way of calculating it?
Start with a drawing: rear view of a car in a turn. Draw the forces and where they act, too
 

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