Finding gravitron rotational frequency

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Homework Help Overview

The problem involves a scenario in an amusement park ride where passengers are inside a rotating cylinder. The goal is to determine the minimum rotational frequency required for passengers to remain safely against the wall after the floor drops away. The subject area includes concepts of friction, centripetal acceleration, and forces acting on the passengers.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the relevant forces, including weight, static friction, and normal force, while questioning how to relate these forces without a given mass. There is exploration of equations related to centripetal motion and friction, with some uncertainty about their applicability.

Discussion Status

Participants are actively engaging with the problem, sharing insights about the relationships between forces and discussing the implications of mass on the safety of the ride. Some guidance has been offered regarding the treatment of normal force and friction, leading to further exploration of the problem.

Contextual Notes

There is an emphasis on the coefficients of friction provided and their relevance to the problem, as well as the assumption that the safety of the ride should not depend on the mass of the passengers.

G4e8cko
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Homework Statement


In an old-fashioned amusement park ride, passengers stand inside a 3.0-m-tall, 5.0-m-diameter hollow steel cylinder with their backs against the wall. The cylinder begins to rotate about a vertical axis. Then the floor on which the passengers are standing suddenly drops away! If all goes well, the passengers will “stick” to the wall and not slide. Clothing has a static coefficient of friction against steel in the range 0.60 to 1.0 and a kinetic coefficient in the range 0.40 to 0.70. What is the minimum rotational frequency, in rpm, for which the ride is safe?

Homework Equations



I'm not even certain which equations would be relevant here. Starting with a free body diagram, I can see that the weight force would point down, and the opposing force would have to be static friction so that would point up, and the centripetal acceleration would be due to the normal force from the walls. So N = mv^2/r

(But I don't have a given mass; should I be able to find mass from the given coefficients of friction since friction counters weight in this situation?)

Force of static friction = u * N

(But I don't know how to find N-- is it still opposing mg if it is in the horizontal direction? If so, I still don't know how to find m…)

v= 2π r/T

Also, v = wr, and then I can convert to rpm… Is this even relevant here, given that I don't have a time period to work with anyway?

Are my thoughts so far on the right track or am I way out in left field? Any nudge in the right direction would be greatly appreciated.
 
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G4e8cko said:
But I don't know how to find N

What was wrong with the following?

G4e8cko said:
So N = mv^2/r

The friction coefficient relates a maximal force in the tangential direction of a surface to the normal force. N is still the normal force.
 
Okay... then I guess I'm stuck as to where to go from there. I don't know how'd I'd go about finding normal force without being given mass. I admit that my understanding of friction is not what it needs to be; I can visualize what you're saying, but I can't quite figure out how to relate it back to these formulas. But thank you for the quick reply!
 
But you have the normal force already as a function of the mass. Do not care about what it is at the moment, leave it in the formulas and see what you get when you impose some relevant condition for the people not falling down. This should clearly not depend on the mass or the safety of the attraction would depend on how fat the visitors are.
 
Oh. You're right, they wouldn't want to exclude visitors based on mass!

After reviewing friction a bit more, I have:

Friction opposes gravity here, so Friction = mg

Friction also = m(a sub c)u

So I can substitute one of these friction equations into the other-- divide mass out of both sides so it won't matter, as we discussed-- and solve for v. I think I've got it from there. Thank you so much for your help!
 

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