Centripetal force Rotor-ride problem

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SUMMARY

The discussion centers on calculating the minimum coefficient of friction required for riders on a "Rotor-ride" to avoid slipping down the wall of a vertical cylinder with a radius of 2.0 meters, rotating at 1.1 revolutions per second. The correct approach involves equating the gravitational force to the frictional force, leading to the formula u = mg/(m(v^2/r)). The final calculated coefficient of friction is 0.103. The centripetal force, provided by the wall, is crucial in this scenario, as it is not equal to the gravitational force.

PREREQUISITES
  • Understanding of centripetal force and its calculation (F_n = m(v^2/r))
  • Knowledge of frictional force and its relationship to normal force (F_f = μF_n)
  • Basic principles of rotational motion and forces
  • Ability to manipulate equations involving mass, gravity, and acceleration
NEXT STEPS
  • Study the concept of centripetal acceleration and its applications in circular motion
  • Learn about the role of normal force in different physical scenarios
  • Explore friction coefficients for various materials and their implications in real-world applications
  • Investigate the dynamics of amusement park rides and safety measures related to forces
USEFUL FOR

Physics students, mechanical engineers, and anyone interested in the dynamics of rotational motion and friction in amusement park rides.

Gauss177
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Homework Statement


In a "Rotor-ride" at a carnival, riders are pressed against the inside wall of a vertical cylinder 2.0m in radius rotating at a speed of 1.1 revolutions per second when the floor drops out. What minimum coefficient of friction is needed so a person won't slip down? Is this safe?

Homework Equations


The Attempt at a Solution


I set friction equal to the net force and then solved for mu, which I'm not sure is right or not:

umg = m(v^2/r)
 
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Are you sure about the 2.0m? That seems awfully small compared to the ones I have seen.

In any case, your equation is not correct. The centripetal force is provided by the wall pushing the people inward, not by frcition. The friction keeps them from sliding down the wall.
 
Yeah the book says 2.0 meters.

For the person to not slide down the wall, the force of friction must equal the force of gravity, right? So do I just do:

F_fr = F_g
umg = mg

But then mg cancels out and u = 1? That doesn't seem right.
 
Gauss177 said:
Yeah the book says 2.0 meters.

For the person to not slide down the wall, the force of friction must equal the force of gravity, right? So do I just do:

F_{fr} = F_g
umg = mg

But then mg cancels out and u = 1? That doesn't seem right.

It is not right. The frictional force has no connection to mg in this problem except that it has to be equal to mg to hold the people in place. Your first equation is good. Your second one is not.

Although mg often appears in friction calculations, it is not the force in F_f = μ____. What belongs in the space?
 
Last edited:
I have no idea. :/ I thought friction was just u*normal? But then where does the 1.1 revolutions per second come from? Thanks for the help
 
Ok I figured out how to do this problem

F_f = F_g
mg = uF_n
mg = m(v^2/r)*u
u = .103

thanks olderdan
 
Gauss177 said:
I have no idea. :/ I thought friction was just u*normal? But then where does the 1.1 revolutions per second come from? Thanks for the help

But you do have an idea :smile: It is the normal force and as you have now realized, the normal force in this problem is not equal to mg.

Gauss177 said:
Ok I figured out how to do this problem

F_f = F_g
mg = uF_n
mg = m(v^2/r)*u
u = .103

thanks olderdan

That's it. For anyone else who might be looking here, the normal force in this problem is from the wall pressing in on the people to keep them in circular motion. It is the centripetal force

F_n = m(v^2/r)

which can be seen from the equations in the quote.
 

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