Circular Motion involving a gravitron

In summary, the conversation discusses a question about calculating the normal force of a gravitron. The equation mv^2/r is used to solve the problem, but there is confusion about the angle involved. It is explained that the angle between the track and the ground is the same as the angle in the vector triangle, and that the normal force must have a vertical component to lift the couch. The correct angle is determined using geometry, and it is noted that the vertical component of the normal force will be greater than the weight force when the couch slides up.
  • #1
Jimmy87
686
17

Homework Statement



I have attached questions about gravitron. I'm struggling with question 2 about calculating the normal force of the gravitron.

Homework Equations



mv^2/r

The Attempt at a Solution



I know the answer so I can figure it out as I know it involves setting the Ncos(62) = mg (N = normal force) but I don't get how you know the angle involved is 62 as it only gives you the angle the track makes with the floor?

Also, please could someone explain why the track is tilted as appose to being vertically upright and what this has to do with enabling the track to slide up when its rotating?
 

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  • Physics Gravitron Questions.docx
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  • #2
Jimmy87 said:
I know the answer so I can figure it out as I know it involves setting the Ncos(62) = mg (N = normal force) but I don't get how you know the angle involved is 62 as it only gives you the angle the track makes with the floor?
The couch is attached to the track, so it makes the same angle. (Is that your question?) Have you drawn yourself a free body diagram of the person?

Also, please could someone explain why the track is tilted as appose to being vertically upright and what this has to do with enabling the track to slide up when its rotating?
The normal force must have a vertical component to lift the person/couch. If it were upright, the weight could not be supported or lifted.
 
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  • #3
Doc Al said:
The couch is attached to the track, so it makes the same angle. (Is that your question?) Have you drawn yourself a free body diagram of the person?


The normal force must have a vertical component to lift the person/couch. If it were upright, the weight could not be supported or lifted.

Thanks Doc Al. I have drawn a free body diagram and attached it. I have resolved the normal force into components and labeled what I think each of them do. Regarding the angle, I know from the answer that one of the angles in that vector triangle I have drawn must be 62 degrees but how do you know this? How can you show that the angle between the track and the ground is the same as the angle in that vector triangle?
 

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  • Free Body Diagram.jpg
    Free Body Diagram.jpg
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  • #4
Jimmy87 said:
Thanks Doc Al. I have drawn a free body diagram and attached it. I have resolved the normal force into components and labeled what I think each of them do.
Good.

Regarding the angle, I know from the answer that one of the angles in that vector triangle I have drawn must be 62 degrees but how do you know this? How can you show that the angle between the track and the ground is the same as the angle in that vector triangle?
The key is to recognize that the angle that the normal makes with the vertical is the same angle that the track makes with the horizontal. That is true because the track and the normal are always perpendicular. One way of seeing that would be to use a bit of triangle geometry or trig. If you label all the angles, I could walk you through it.

Even easier might be this. Imagine that the track was on a hinge that could move through any angle θ, instead of being fixed at 62 degrees. Now lay the track flat so that θ = 0. What angle does the normal make with the vertical? 0, of course, since it points straight up. Now increase the angle to 1 degree. Can you see that the normal must move 1 degree to the vertical? No matter what angle the track makes with the horizontal, the normal will make that same angle with the vertical.

Make sense?
 
  • #5
Doc Al said:
Good.The key is to recognize that the angle that the normal makes with the vertical is the same angle that the track makes with the horizontal. That is true because the track and the normal are always perpendicular. One way of seeing that would be to use a bit of triangle geometry or trig. If you label all the angles, I could walk you through it.

Even easier might be this. Imagine that the track was on a hinge that could move through any angle θ, instead of being fixed at 62 degrees. Now lay the track flat so that θ = 0. What angle does the normal make with the vertical? 0, of course, since it points straight up. Now increase the angle to 1 degree. Can you see that the normal must move 1 degree to the vertical? No matter what angle the track makes with the horizontal, the normal will make that same angle with the vertical.

Make sense?

Thanks again Doc Al! Kind of making sense. I have drawn another FBD (attached) and I think I have figured out the angle using a bit of geometry, please could you check to see if it's correct? I have extended the weight force in purple. If the angle between the track and the ground is 62 then the other angle (a) must be 28. I think I am right in saying that because there are two straight lines crossing that a and b are alternate interior angles? Angle c must be 90 minus 28 which is 62 degrees. Is that how you prove it or is that a very long way of doing it?

Also, am I right in saying that the vertical component of the normal force will be greater than the weight force when the couch slides up?
 

Attachments

  • Free Body Diagram 2.jpg
    Free Body Diagram 2.jpg
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  • #6
Jimmy87 said:
Thanks again Doc Al! Kind of making sense. I have drawn another FBD (attached) and I think I have figured out the angle using a bit of geometry, please could you check to see if it's correct? I have extended the weight force in purple. If the angle between the track and the ground is 62 then the other angle (a) must be 28. I think I am right in saying that because there are two straight lines crossing that a and b are alternate interior angles? Angle c must be 90 minus 28 which is 62 degrees. Is that how you prove it or is that a very long way of doing it?
That's pretty much it. Here's my version. Call the angle that track makes with the horizontal θ, instead of a specific number. Angles b and c must add to 90, since they make a right angle. Same for angles a and θ. But you know that a = b, so therefore c = θ.

Symbolically:
b + c = 90
a + θ = 90
thus b + c = a + θ
but b = a, so:
c = θ

Also, am I right in saying that the vertical component of the normal force will be greater than the weight force when the couch slides up?
Yes.
 
  • #7
Doc Al said:
That's pretty much it. Here's my version. Call the angle that track makes with the horizontal θ, instead of a specific number. Angles b and c must add to 90, since they make a right angle. Same for angles a and θ. But you know that a = b, so therefore c = θ.

Symbolically:
b + c = 90
a + θ = 90
thus b + c = a + θ
but b = a, so:
c = θ


Yes.

Thank you very much!
 

FAQ: Circular Motion involving a gravitron

What is circular motion involving a gravitron?

Circular motion involving a gravitron is a type of rotational motion where an object or particle moves along a circular path around a fixed point, known as the center of rotation. The gravitron is a ride commonly found in amusement parks that simulates circular motion by spinning riders around a central axis.

What causes circular motion involving a gravitron?

Circular motion involving a gravitron is caused by the centripetal force, which is the force that pulls an object towards the center of rotation. In the case of a gravitron ride, this force is provided by the rotation of the ride and the harnesses that keep riders in place.

How does the speed of a gravitron ride affect circular motion?

The speed of a gravitron ride affects circular motion by increasing or decreasing the centripetal force acting on the riders. As the ride spins faster, the centripetal force increases, causing riders to experience a greater sensation of circular motion. When the ride slows down, the centripetal force decreases, resulting in a less intense experience.

What is the difference between centripetal and centrifugal force in circular motion?

Centripetal force is the force that pulls an object towards the center of rotation in circular motion, while centrifugal force is the apparent outward force experienced by an object in circular motion. In reality, there is no such thing as centrifugal force, but it is often used as a simplification to explain the sensation of being pulled outwards in circular motion.

How is the motion of objects in circular motion involving a gravitron affected by their mass?

The mass of an object in circular motion has no effect on its motion in a gravitron ride. This is because the centripetal force is not dependent on the mass of the object, but rather on the speed and radius of the circular path. This is why riders of different weights can experience the same sensation of circular motion on a gravitron ride.

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