Circular motion and gravitation

AI Thread Summary
The discussion focuses on calculating the banking angle for a vehicle navigating a curve of radius 200m at a speed of 90km/h without relying on friction. The key point is that only the normal force (Fn) contributes to the centripetal force in the horizontal direction, while gravity (Fg) acts vertically and does not have a horizontal component. The correct approach involves using the equation ΣFc = mac, where only the horizontal component of the normal force, Fnsin(theta), is included. The confusion arises from comparing this scenario to inclined plane problems, where gravity has a parallel component; however, in banked curves, the centripetal acceleration is horizontal, making gravity irrelevant to the horizontal force balance. Understanding these distinctions is crucial for solving the problem accurately.
Inertialforce
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Homework Statement


Traffic is expected to move around a curve of radius 200m at 90km/h. What should be the value of the banking angle if no dependence is to be placed on friction?


Homework Equations


ΣFc = mac


The Attempt at a Solution


For this question what I did first was draw a top view of the situation, then I drew a side view of the same situation but with vectors to show what forces were acting on the car as it was going through the bank (free body diagram). As it turns out (since it says that no dependence is placed on friction) the only forces acting on the car along the bank are the forces Fn and Fg.

My question is when I put it into the centripetal force equation, what force do I incorporate into the equation?

For example is it:
ΣFc = mac
Fnsin(theta) = mac

or is it:
ΣFnsin(theta) + mgsin(theta) = mac
 
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Hi Inertialforce,

Inertialforce said:

Homework Statement


Traffic is expected to move around a curve of radius 200m at 90km/h. What should be the value of the banking angle if no dependence is to be placed on friction?


Homework Equations


ΣFc = mac


The Attempt at a Solution


For this question what I did first was draw a top view of the situation, then I drew a side view of the same situation but with vectors to show what forces were acting on the car as it was going through the bank (free body diagram). As it turns out (since it says that no dependence is placed on friction) the only forces acting on the car along the bank are the forces Fn and Fg.

My question is when I put it into the centripetal force equation, what force do I incorporate into the equation?

For example is it:
ΣFc = mac
Fnsin(theta) = mac

or is it:
ΣFnsin(theta) + mgsin(theta) = mac

First determine what direction the centripetal acceleration ac is in. Then, in your centripetal force equation, you find the components of all forces in that direction; those components go in the centripetal force equation. What do you get?

(That is, what is the component of the normal force in the direction ac is pointing, and the component of the gravity force in the direction ac is pointing?)
 
alphysicist said:
Hi Inertialforce,



First determine what direction the centripetal acceleration ac is in. Then, in your centripetal force equation, you find the components of all forces in that direction; those components go in the centripetal force equation. What do you get?

(That is, what is the component of the normal force in the direction ac is pointing, and the component of the gravity force in the direction ac is pointing?)

In my free body diagram I have Fnsin(theta) and mgsin(theta) pointing towards the direction of my centripetal acceleration. But what I do not understand is that, I know I am supposed to write down all the forces pointing in the direction of the centripetal acceleration in my equation which would make:

ΣFc = mac
Fnsin(theta) + mgsin(theta) (because they are both pointing left to the direction of the centripetal acceleration)

However, in my physics textbook they have a example that is almost identical but in their free body diagram they only showed or expanded upon the forces of Fn (the free body diagram only includes the vectors Fn, Fncos(theta), Fnsin(theta) , and mg. I was just wondering why they do not include the cos and sin vectors for mg as well and also why they do not include mgsin(theta) or mgcos(theta) in the banked curve examples/questions that they show.
 
Inertialforce said:
In my free body diagram I have Fnsin(theta) and mgsin(theta) pointing towards the direction of my centripetal acceleration. But what I do not understand is that, I know I am supposed to write down all the forces pointing in the direction of the centripetal acceleration in my equation which would make:

ΣFc = mac
Fnsin(theta) + mgsin(theta) (because they are both pointing left to the direction of the centripetal acceleration)

Here is the important part: the centripetal acceleration is to the left, so it is a horizontal acceleration. But the gravity force has no component in the horizontal direction; it is a vertical force.


(What confuses many people is the similarity in the diagrams for these problems and for problems involving boxes sliding down inclined planes. But the problems are different in that for the boxes, the acceleration is down the incline, and gravity has a component parallel to the incline.

But for these banked curve problems, the acceleration is horizontal, and gravity has no horizontal component.)
 
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