Circular Motion Question (Possibly Easy?)

In summary: This is a simple newtons law problem, so you should be able to take it from here.In summary, the correct banking angle for the highway curve with a radius of 420m and traffic moving at 73.0 km/hr is determined by using the formula a=(v^2)/r and setting up a free body diagram with the normal force and weight. The mass is not needed in the calculations as it cancels out, and the angle can be solved for using the components of the normal force and weight. Friction does not play a role in this problem.
  • #1
BlakeGriffin
8
0

Homework Statement


A highway curve of radius 420m is designed for traffic moving at a speed of 73.0 km/hr .

What is the correct banking angle of the road?

Homework Equations


V=(2(pi)(r)/T)
a=(v^2)/r

The Attempt at a Solution


I feel like this is an easy question but for some reason I can't get it.

r=420m
v=73 mi/hr which is 20.3 m/s

I was going to use a free body diagram to find the normal force then use the cos and sin stuff to find the angle but since the mass is not given I don't know what to do.

I don't know where to go exactly? Can anyone just tell me what I'm missing here?
 
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  • #2
A body that moves in a circle needs a net force to move in this circle. If the circle has a radius R and the body moves with a speed v then the force needed to keep the body in the circle is given by mv^2/r, using Newtons first law and sentriple aceleration. This is one way to write this force

F=mv^2/r

So, what force is it that keeps it in the circle? Well there is no friction, so we need an angle and a component from the normal force. Do you know how to find this component? Find the component in therms og m, g and the angle and sustitute for F. Notice that the m-s cancel, so you don't need them. Then solve for the angle and youre done.
 
  • #3
Basically, for a flat road, friction is what provides the centripetal force that keeps the car moving in a circle. If you bank the curve, then there is also a component of the weight that is parallel to the incline that helps you out as well. Draw the free body diagram and set up the equations, and you should see that mass doesn't matter (it cancels from both sides of the equation).
 
  • #4
Btw, your first equation is not relevant
 
  • #5
So is this what the free body diagram looks like then?

http://img851.imageshack.us/img851/3382/232.jpg

Dash marked lines are the components of normal force.
 
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  • #6
I was having trouble interpreting that FBD, but if the vertical force is weight and the oblique one is the normal force, then that looks right. So, is there no friction in this problem? If not, then the FBD is complete.
 

FAQ: Circular Motion Question (Possibly Easy?)

What is circular motion?

Circular motion is a type of motion in which an object moves along a circular path. This means that the object's distance from a fixed point remains constant while its direction changes continuously.

What causes circular motion?

Circular motion is caused by a centripetal force, which is a force directed towards the center of the circular path. This force is necessary to keep an object moving in a circular path and prevents it from moving in a straight line.

How is circular motion different from linear motion?

Circular motion involves a change in direction, while linear motion involves a change in position. In circular motion, the object's distance from a fixed point remains constant, while in linear motion, the object's distance from a starting point changes.

What is the difference between uniform and non-uniform circular motion?

Uniform circular motion is when an object moves at a constant speed along a circular path, while non-uniform circular motion is when the speed of the object changes along the circular path. In non-uniform circular motion, the object experiences a change in velocity, while in uniform circular motion, the velocity remains constant.

How is centripetal force related to circular motion?

Centripetal force is necessary for circular motion because it is responsible for keeping an object moving along a circular path. It acts as a "center-seeking" force, pulling the object towards the center of the circular path and preventing it from flying off in a straight line.

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