Car moving along a banked curve with friction

In summary, the car will require friction to move along the curve. The amount of friction required is dependent on the speed and angle of the curve.
  • #1
Dr4c0
7
0
car moving along a banked curve with friction (solved)

first off, thanks to whoever helps me. you're a life saver. i could just copy it from a friend, but i want to be skilled enough for the AP Physics B exam. so yeah... i just want to understand what i have to do. the logic with this is killing me.
ok here's the problem:
A 1200-kg car rounds a curve of radius 67m banked at an angle of 12 degrees. If the car is traveling at 95 km/h, will a friction force be required? If so, how much and in what direction?
ok, here's what i got so far. first, i converted 95 km/h to 26.388... m/s. then, i found a formula in the book for things with no friction required: tan (theta) = (v^2)/(rg). so i plugged in the angle, radius, and gravity constant to see what speed would be necessary for no friction required. i got 11.8 m/s. nowhere near. so i now have that friction is required. simple enough.
so now i need to find out how much friction force is needed. i drew a diagram to help me figure out how weight, normal force, friction force, and centripetal force are related as vectors. i understand centripetal force and weight are constant in this case. i know i have to find the friction force as a vector since the coefficient of friction isn't provided, so i can't find it directly from normal force. thing is though, normal force and friction force affect each other, and i have no clue how to figure out normal force in this case. i tried messing around with the vectors and solving for friction force by pythagorean theorem, sin, and cos, but i ended up getting three different answers... i am massively confused. assistance would be GREATLY appreciated.
 
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  • #2
This is a circular motion question, the car is moving in a circle so is therefore accelerating so there must be a resultant (centripetal) force directed inwards (due to Newton's second law) which is equal to the frictional force.

work out the horizontal component of v then use :

F = mv^2/r
 
  • #3
i wish it were that easy. that would be true if the curve was flat, but the curve is banked. the friction force is at an angle.

physicsprob.jpg
 
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  • #4
There is no friction force pointing out of the circle. The only frictional force is pointing in because it keeps the car in the circle. The normal forces and friction forces are vectors and can be broken up into horizonal and vertical components.

Then you can say that the sum of all vertical forces(weight, y component of normal force, and y component of frictional force) = 0 because there is no vertical acceleration.

Sum of all horizonal forces = mv^2/r and go from there.
 
  • #5
Your diagram contains a 'centrifugal' force!

The method I said should work, just convert everything to ms^-1
Then work out the centripetal force, and resolve it down the slope to get the frictional force.
 
  • #6
very, very good!
...but how do i go about splitting normal force and friction force into horizontal and vertical vectors? :confused:
 
  • #7
newcool said:
There is no friction force pointing out of the circle. The only frictional force is pointing in because it keeps the car in the circle. The normal forces and friction forces are vectors and can be broken up into horizonal and vertical components.

Then you can say that the sum of all vertical forces(weight, y component of normal force, and y component of frictional force) = 0 because there is no vertical acceleration.

Sum of all horizonal forces = mv^2/r and go from there.

You can't say the sum of all forces = 0 because there is a resultant force on the body as it is accelerating.
 
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  • #8
rho said:
Your diagram contains a 'centrifugal' force!

The method I said should work, just convert everything to ms^-1
Then work out the centripetal force, and resolve it down the slope to get the frictional force.

centrifugal force is force pointing out from the circle. the inertia of the car provides that. it's not a factor.

converting all the forces into acceleration won't do anything. i'll just have accelerations in all different directions instead of forces. that won't solve for any of the values.

unless I'm misunderstanding what you're saying?
 
  • #9
rho said:
You can't say the sum of all forces = 0 because there is a resultant force on the body as it is accelerating.

the sum of all vertical forces = 0. this is because the car is not accelerating up or down. this means the net force is zero vertically.

however, the car is accelerating horizontally by going in a circle (centripetal acceleration). that's why the horizontal accelerations and forces equal the centripetal acceleration and forces because that is the net acceleration and force.
 
  • #10
The answer should just be: F(friction)= F(centripetal)/ cos 12

unless i misunderstand this question.
 
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  • #11
...wow. i feel like a complete moron. thanks rho! ^.^
 
  • #12
rho said:
The answer should just be: F(friction)= F(centripetal)/ cos 12
unless i misunderstand this question.
There is also the slope component of the mass of the car providing some of the centripetal force. That should also be taken into account.
 
  • #13
Fermat said:
There is also the slope component of the mass of the car providing some of the centripetal force. That should also be taken into account.

Isn't that considered by the fact that we're taking the friction force in consideration with the angle (cos 12)?
 
  • #14
Dr4c0 said:
Isn't that considered by the fact that we're taking the friction force in consideration with the angle (cos 12)?
The forces acting down the slope are: Friction and the slope component of the mass of the car, mg.sinα.
This is equal to the slope component of the centripetal force, Fc. viz.

Fr + mgsinα = Fc.cosα
Fc = (Fr/cosα + mg.tanα)
mv²/r = (Fr/cosα + mg.tanα)
v² = (Fr.r/m.cosα + (g/r).tanα)
========================

and if there is no friction, then v_crit is given by,
v²_crit = (g/r).tanα
===============

our standard result.
 

1. How does friction affect a car moving along a banked curve?

Friction is a force that opposes motion, so it can affect the car's speed and direction as it moves along the banked curve. If there is too much friction, the car may slow down or even slide off the curve. However, the right amount of friction can actually help the car stay on the curve without sliding off.

2. What factors contribute to the amount of friction on a banked curve?

The amount of friction on a banked curve depends on the surface materials of the road and the tires, as well as the speed and weight of the car. Additionally, the angle of the banked curve and the presence of any external forces, such as wind or rain, can also affect the amount of friction.

3. How is the angle of the banked curve determined for a car to safely travel without slipping or sliding?

The angle of a banked curve is determined by considering the speed of the car and the force of gravity. The goal is to have the centripetal force (which keeps the car moving in a circular path) equal to the force of gravity pulling the car down the curve. This can be achieved by adjusting the angle of the curve until the forces are balanced.

4. Can a car still move along a banked curve if there is no friction?

Yes, a car can still move along a banked curve without friction, but it may not be able to stay on the curve without sliding off. This is because the force of friction helps to keep the car from slipping and provides the necessary centripetal force to keep the car moving in a circular path.

5. How does the speed of the car affect its movement along a banked curve with friction?

The speed of the car plays a crucial role in its movement along a banked curve. If the car is moving too slowly, there may not be enough centripetal force to keep it on the curve, and it may slide off. On the other hand, if the car is moving too quickly, it may experience too much centrifugal force, causing it to slide outwards. Therefore, the speed must be carefully considered and adjusted for safe travel along a banked curve.

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