Angle needed on banked corner of road.

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In summary: There's a link at the bottom of the page. In summary, the author is explaining how to calculate the normal force on a car travelling around a corner. The first equation is the centripetal force, and the second equation is the equation to keep the car from moving.
  • #1
Lachlan1
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Homework Statement



this example is in the txtbook so i know the answer, but i don't really get the second part.

The road needs to be at a banked angle so the car traveling at 13.4m/s can go around with no friction needed, the radius of the corner is 35m.



Homework Equations



the given contructed equations are
Fr=nsinө = (mv^2)/r i get this part, just the horizontal component of the normal force, which is the centripedal force.

then they use
Fy=ncosө – mg = 0
which i can see from the diagram is the vertical component of the normal force, less the weight force of the car. Why do they use this though?

they then divide the two equations.


The Attempt at a Solution



i got the first equation, and initially tried to write n, the normal force as mgcosө, and then substitute it into the first equation. Why is this not the normal force? like for an inclined plane example? and why do they subtract the car weight force from the verticle component of the normal force?

thanks
 
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  • #2
Lachlan1 said:
...tried to write n, the normal force as mgcosө...

Try N = mg/cos θ... :wink:
 
  • #3
Lachlan1 said:
then they use
Fy=ncosө – mg = 0
which i can see from the diagram is the vertical component of the normal force, less the weight force of the car. Why do they use this though?
Is the car accelerating in the vertical (y) direction? If it is not accelerating in the y-direction, then the y-components of all the forces involved must add up to zero.
i got the first equation, and initially tried to write n, the normal force as mgcosө, and then substitute it into the first equation. Why is this not the normal force?
The car is accelerating in the horizontal direction (which can be expressed as the resultant force). This resultant force has to come from somewhere. So the normal force not only involves the force of gravity (in the vertical direction) but the resultant force too (in the horizontal direction).

I suggest starting with a free body diagram (FBD). By looking at the forces in the FBD, it should be more clear. :smile:
like for an inclined plane example?
In most inclined plane examples, the objects are not accelerating with respect to the surface of the plane (they may or may not be accelerating parallel to it, but there usually is no acceleration component perpendicular to the plane). This problem is different.
and why do they subtract the car weight force from the verticle component of the normal force?
Is the car accelerating up or down? :wink:
 
  • #4
thanks for the replies. No, the car is not accelerating in the verticle direction, so i can see why the forces in the verticle must equal zero. I have been looking at a link at the bottom of the page to a question posted on here over a year ago which was asking the same question i am.
 
  • #5
The first equation comes from centripetal force which you already figured out.
The second equation is the equation to keep The Car from moving in the air.
So, consider a box on floor => for that you would do N = mg
In this case. N = mgcostheta. because you don't want car to fly from the banked surface.

Just look at diagram(red thing is car(best i could draw in paint))
but
first eqn. is eqn for x-comp.
second eqn is eqn for y-comp

Also note: Normal is always perpendicular to surface and Force due to Gravity is always downwards
 

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  • #6
utkarsh1 said:
The first equation comes from centripetal force which you already figured out.
The second equation is the equation to keep The Car from moving in the air.
So, consider a box on floor => for that you would do N = mg
In this case. N = mgcostheta. because you don't want car to fly from the banked surface.

Sorry utkarsh1, but you haven't got your FBD quite right. The normal force is definitely not mgcosθ. That would only be true if there was no other acceleration happening that has a component parallel to the normal force. In this problem, the car is accelerating such that the acceleration is not perpendicular to the normal force. So mgcosθ, by itself, is not the normal force for this problem.

Lachlan1, Try this FBD (if your textbook doesn't already have its own FBD).
 

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FAQ: Angle needed on banked corner of road.

1. What is a banked corner of road?

A banked corner of road is a curved section of road that is built at an angle to allow vehicles to maintain speed and stability while turning.

2. Why is it important to have a banked corner of road?

Having a banked corner of road is important for the safety of drivers and passengers. It allows vehicles to turn smoothly and reduces the risk of accidents or skidding.

3. What factors determine the angle needed for a banked corner of road?

The angle needed for a banked corner of road is determined by the speed of vehicles, the radius of the curve, and the coefficient of friction between the tires and the road surface.

4. How is the angle calculated for a banked corner of road?

The angle needed for a banked corner of road can be calculated using the formula: angle = arctan (v^2/g x r), where v is the speed of the vehicle, g is the acceleration due to gravity, and r is the radius of the curve.

5. What are the potential risks of having an incorrect angle on a banked corner of road?

If the angle on a banked corner of road is too steep, it can cause vehicles to lose control and potentially lead to accidents. If the angle is too shallow, it may not provide enough support for vehicles and also increase the risk of accidents.

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