Solving the Angle of a Rolling Penny

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Homework Help Overview

The problem involves a penny rolling on a table in a circular path, requiring the determination of the angle \Theta that the axis of the penny makes with the horizontal. The context includes parameters such as the radius of the coin, the radius of the circular path, and the velocity of the penny.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the use of a free body diagram to analyze the forces acting on the penny, including weight, normal force, and friction. There is a focus on the role of acceleration in the context of circular motion, with questions about how to incorporate it into the analysis.

Discussion Status

The discussion is ongoing, with participants exploring the implications of the free body diagram and the necessity of including acceleration in their reasoning. Some guidance has been offered regarding the relationship between forces and acceleration, but no consensus or resolution has been reached.

Contextual Notes

Participants note the absence of mass in the problem statement and express uncertainty about how to proceed without it. There is an acknowledgment of the assumptions regarding the penny's motion and the forces involved.

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Homework Statement


If you start a penny rolling on a table with care, you can make it roll in a circle. The coin leans inward with its axis tilted. The radius of the coin is r, the radius of the circular path it follows is R, and velocity is v. Assuming that the coin does not slip, find the angle \Theta that the axis makes with the horizontal

The answer is given as
tan\Theta=(3v2)/(2gR)

I always have problems figuring out how to start the problems, but the answer usually becomes clear after I get past the first step. The only equation that I can think of that would help is I=.5mb2, but since mass isn't mentioned in the problem it seems useless.

So far what I have done is draw a free body diagram of the penny with the force of the penny's weight acting straight down, the normal force acting straight up, and frictional force directing it toward the center of the circular path it follows.

Where would be a good place to start?
 
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davesface said:
So far what I have done is draw a free body diagram of the penny with the force of the penny's weight acting straight down, the normal force acting straight up, and frictional force directing it toward the center of the circular path it follows.

Where would be a good place to start?

Hi davesface! :smile:

You've started in the right place, but you've left out the acceleration.

(you don't like acceleration, do you? :wink:)
 
I have nothing against acceleration, but that free body diagram was the hint that we got about the problem, and it did not include acceleration. I would assume that the acceleration would be toward the center of the circle, though.
 
davesface said:
I have nothing against acceleration, but that free body diagram was the hint that we got about the problem, and it did not include acceleration. I would assume that the acceleration would be toward the center of the circle, though.

Hi davesface! :smile:

An FBD can include acceleration.

(This is because an FBD works because of Newton's second law … force = mass times acceleration … so acceleration-times-mass can go in the FBD just like force :wink:)

Yes, you're right … the acceleration is toward the center of the circle ("centripetal") … its magnitude is v2/r.

Multiply it by the mass, bung it in the FBD and solve! :smile:
 
Good stuff.
 

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