Need Help Understanding Concepts of Centripetal Force.

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Discussion Overview

The discussion revolves around the concepts of centripetal force and its relationship with friction and inertia, particularly in the context of a car navigating a circular path. Participants explore the nature of forces acting on the car, the role of friction in providing centripetal acceleration, and the implications of inertia in circular motion.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant asserts that friction between the tires provides the necessary centripetal force for a car turning in a circular arc, questioning what force counteracts this centripetal force.
  • Another participant clarifies that a net force is required to change the car's path, which is provided by friction, and emphasizes that no additional force is needed to "hold the car in its path."
  • Some participants express confusion about the necessity of an opposing force to centripetal force, suggesting that without it, the car would move toward the center of the circle.
  • A participant explains that the acceleration is directed toward the center, while the velocity is tangential, indicating that the force causes a change in direction rather than a movement toward the center.
  • Another participant connects the concept of tangential velocity to inertia, suggesting that inertia prevents the car from "falling in" toward the center of the circle.
  • There is a discussion about centrifugal force, with some participants noting it as a fictitious force arising from inertia when viewed from a rotating frame of reference, while others recommend understanding the situation from an inertial frame without relying on this concept.

Areas of Agreement / Disagreement

Participants exhibit disagreement regarding the necessity and interpretation of opposing forces in circular motion. While some assert that friction is the sole centripetal force, others question the implications of inertia and centrifugal force, leading to an unresolved discussion on these concepts.

Contextual Notes

There are limitations in the discussion regarding the definitions of forces and the frames of reference being used. The relationship between centripetal force, friction, and inertia remains a point of contention, with various assumptions about the nature of forces in circular motion not fully explored.

ha9981
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Now as I understand, a force must be present to cause centripetal acceleration. So as a car goes around a circular arc it is friction between the tires which causes centripetal acceleration. So since the car is turning around the curve the friction will be perpendicular to the instantaneous velocity and therefore towards the center of the arc.

So with this I am guessing Ff must be equal to mv2/r or any other form of the centripetal force eqn. But as I see it friction force and centripetal force are the same in this situation and it is directed to the center, now I ask what is holding the car in its path. To me it seems its friction, but isn't friction causing centripetal force. So what is the force in the opposite direction? I know it has to be equal in magnitude. I was thinking centrifugal but not to sure how it works. From what i remember that centrifugal originates from inertia, so if there was no centripetal force able to be exerted the object in uniform circular motion will go off on a tangent.

Then I read this: "Caution: In doing problems with uniform circular motion, you may be tempted to include an extra outward force of magnitude mv2/r to keep the body "out there" or to "keep it in equilibrium". This outward force is called the centrifugal force (fleeing from the center). Resist this temptation, because this approach is simply wrong. In an inertial frame of reference there is no such thing as centrifugal force."
 
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You don't need anything to "hold the car in its path". You do need a net force to change the path--to make it go in a circle. In your example, that net force is provided by friction.
 
I am not to sure what you are saying.

I know there is a centripetal force, and because of that there must be another force or the car will go into the center of the circle, or am i seeing this all wrong?
 
ha9981 said:
I know there is a centripetal force, and because of that there must be another force or the car will go into the center of the circle, or am i seeing this all wrong?
You are seeing it wrong, but it's a bit tricky. The acceleration is toward the center, not the velocity.

A force doesn't necessarily make something move in the direction of the force. What it does is provide an acceleration (a change of velocity) in the direction of the force. If the acceleration is perpendicular to the object's direction of motion, the force just makes it turn sideways in a circle, not move toward the center of the circle.

Also: If there were another force acting opposite to the centripetal force, canceling it out, then the net force on the object would be zero. It would just keep moving in a straight line--not around in a circle.
 
Welcome to PF!

Hi ha9981! Welcome to PF! :smile:
ha9981 said:
I know there is a centripetal force, and because of that there must be another force or the car will go into the center of the circle, or am i seeing this all wrong?

The centripetal force is the friction force.

Because of that force, the car does go into the centre …

only its tangential velocity prevents it from "falling in".

This is what good ol' Newton discovered about gravity …

if you throw an apple horizontally, it falls … if you throw it hard enough, it still falls at the same rate, but it goes so fast sideways that it stays the same distance from the centre of the Earth … in other words it goes into (very-near-Earth!) orbit. :wink:
 


tiny-tim said:
The centripetal force is the friction force.

Because of that force, the car does go into the centre …

only its tangential velocity prevents it from "falling in".

When you refer to "tangential velocity" is this basically inertia? The inertia the car is feeling because of tangential velocity at each point in the curve keeps it from falling in?

Is this like :
Doc Al said:
What keeps the bucket and water "up" is their inertia. They are being swung in a circle.

Also is the inertia based force centrifugal force? Because I read that it is fictitious since its based on inertia which doesn't exactly make it a force but just following Newtons laws.
 


ha9981 said:
Also is the inertia based force centrifugal force? Because I read that it is fictitious since its based on inertia which doesn't exactly make it a force but just following Newtons laws.
If you wish to view things from the rotating frame of reference, you would add a centrifugal force (not a "real" force, just an artifact of using an accelerating frame of reference) in order to apply Newton's laws.

But I recommend that you try to understand things from the usual inertial frame of reference and don't rely on the "crutch" of the centrifugal force. (At least until you get to more advanced courses, where you'll need to use rotating frames.)
 
ha9981 said:
When you refer to "tangential velocity" is this basically inertia?

Yeah, basically … Newton's first law means it wants to keep going in a straight line.
Also is the inertia based force centrifugal force?

There's no "inertia based forces" … inertia is inertia, and force is force, and they're more-or-less opposites.

(there are so-called "inertial forces", also called "fictitious forces", but that only means forces whose strength doesn't depend on charge or velocity but only on mass, which is another word for inertia)
 

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