Circular Motion Force at Point A: Stunt Car on Frictionless Track

In summary, the problem involves a stunt car driver navigating a frictionless track with a radius of 9.9 m and a mass of 1800 kg. The driver is able to barely stay on the track at the top of the loop. To find the force of the car on the track at point A, we must first calculate its required speed at the top of the loop by using the equation V2/R. Then, using conservation laws, we can find the force exerted by the car on the track.
  • #1
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Homework Statement


In the figure, a stunt car driver negotiates the frictionless track shown in such a way that the car is barely on the track at the top of the loop. The radius of the track is 9.9 m and the mass of the car is 1800 kg. Find the force of the car on the track when the car is at point A

http://session.masteringphysics.com/problemAsset/1107086/1/7.10.jpg"

Homework Equations



Accelaration(radius) V2/R F=ma


The Attempt at a Solution



massxacceleration =1800kg x V2/9.9m ... v2=1800kg/9.9 =181 .. v=13.4 m/s

F=1800kg x (13.4)2/9.9

Can someone help me please.. what am I doing wrong?
 
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  • #2
Is the loop vertical? Is the car traveling on an inclined slope?
 
  • #3
sorry for the confusion i included a picture link for the problm
 
  • #4
If the track is frictionless then his trajectory is ballistic; he can't use the engine to accelerate because the tires have no friction with the track.

The condition posed is that the car is "barely on the track at the top of the loop". So work out its required speed there. Then use whatever conservation laws spring to mind.
 
  • #5


I would like to clarify that circular motion is a complex concept that involves not only the mass and acceleration of an object, but also the centripetal force acting on the object. In this scenario, the car is moving in a circular path, which means it is constantly changing direction and therefore experiencing a centripetal acceleration towards the center of the loop. This acceleration is caused by a force known as the centripetal force, which is provided by the track in this case.

To find the force of the car on the track at point A, we need to use the equation F=ma, where m is the mass of the car and a is the centripetal acceleration. The centripetal acceleration can be calculated using the equation a=v^2/r, where v is the speed of the car at point A and r is the radius of the loop.

Using the given information, we can calculate the speed of the car at point A using the equation v=sqrt(gr), where g is the acceleration due to gravity and r is the radius of the loop. Plugging in the values, we get v=sqrt(9.8 m/s^2 x 9.9 m)= 9.9 m/s.

Now, we can calculate the centripetal acceleration using the equation a=v^2/r, which gives us a=(9.9 m/s)^2 / 9.9 m= 9.9 m/s^2.

Finally, we can calculate the force of the car on the track at point A using the equation F=ma, which gives us F=1800 kg x 9.9 m/s^2= 17,820 N.

Therefore, the force of the car on the track at point A is 17,820 N. It is important to note that this force is provided by the track and is necessary to keep the car moving in a circular path. Without this force, the car would move in a straight line tangent to the loop.
 

FAQ: Circular Motion Force at Point A: Stunt Car on Frictionless Track

What is circular motion force?

Circular motion force is the force that acts on an object moving in a circular path. It is always directed towards the center of the circle and is responsible for keeping the object moving in a curved path.

How is circular motion force calculated?

Circular motion force can be calculated using the formula F = mv²/r, where F is the force, m is the mass of the object, v is the velocity, and r is the radius of the circle.

What is the relationship between circular motion force and speed?

The circular motion force is directly proportional to the speed of the object. This means that as the speed increases, the force also increases. Similarly, if the speed decreases, the force decreases as well.

What is the role of centripetal force in circular motion?

Centripetal force is another term used to describe circular motion force. Its role is to keep the object moving in a circular path and prevent it from moving in a straight line tangent to the circle.

What are some real-life examples of circular motion force?

Some examples of circular motion force include the force exerted by a car's tires on the road while taking a turn, the force exerted by a satellite on the Earth in its orbit, and the force exerted by a spinning top on the surface it is spinning on.

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