Max static friction witout mass or normal force?

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Homework Help Overview

The problem involves determining the maximum distance from the center of a turntable at which a coin will not slide off, given the coefficient of static friction and the turntable's rotational speed. The subject area includes concepts of friction, circular motion, and rotational dynamics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the relationship between static friction and centripetal force, questioning how to approach the problem without knowing the mass or normal force. There are attempts to derive relationships between the variables involved, including the conversion of RPM to radians per second.

Discussion Status

Participants have provided insights into the relationships between the forces and have explored the conversion of units. There is ongoing confusion regarding the transition from angular velocity to linear distance, and some participants have suggested using known equations to relate these quantities.

Contextual Notes

Participants note that the problem originates from the GRE, and there is a reference to an answer key that provides a specific numerical solution, which raises questions about the reasoning leading to that answer.

Gersty
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Homework Statement


The coefficient of static friction between a small coin and a turntable is 0.30. The turntable rotates at 33.3 RPM. What is the max distance from the center of the turntable at which the coin will not slide?

Homework Equations


Fs max =μs (FN)
V = ω (r)

a=(V^2)
-----
r

Fc=m(vt)^2
------
r

The Attempt at a Solution


Didn't get very far. How can this be done without the mass of the coin, or the normal force supporting it? The Force of static friction is the only horizontal force acting on the coin, correct? When the inertia of the coin overcomes this Force of static friction, the coin will slide, correct?
 
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You can think of the frictional force as the centripetal force which keeps the coin in a circular orbit. Therefore, you will see that F=ma=μN=μmg
Notice that the m cancels.

All you need now is just what is the a required?
 
Just did some more research and found the following:

F_cent = m(v^2)/R = F_s_max = (mu_s) · mg ,

giving us

mu_s = (v^2) / gR .

So we figure out what the total horizontal force could be...
F_cent = m(v^2)/R = F_s_max = (mu_s) · mg
Come up with an equality that features quantities we are interested in...
mu_s = (v^2) / gR
and solve for R?

mu_s is dimensionless
g is in m/s^2
and the answers are all in m.

How can I go from RPMs to something that will give me an answer in meters?
 
The SI unit of rotational velocity is radians per second or s^(-1). RPM is revolutions per minute. How many radians in one revolution?
 
You have the equation in your first post! V=omega*r (omega in radians)

You need to convert your RPM into radians/second which will give you omega.
 
There are 2pi radians in one revolution and 60 seconds in one minute, so...
33.3 RPM (2pi rad/1 REV) (1 min/60 s)= 3.49 rad/s!

So I have r = (v^2)/(mu_s)(g)...and I'm no longer thinking straight.
 
According to the answer key, the correct answer is 0.242 m. I'm still confused as to how we go from radians to meters. What obvious thing am I missing??
 
w = 3.49 rad/s is correct. Substitute for V in your equation. Namely V = rw. By the way where does this problem come from? The GRE? I know I have seen it before with these numbers.
 
Yep. It's from the GRE.
So: r =[(3.49rad/s)(r)]^2/[mu_s(g)] ?
 
  • #10
Gersty said:
Yep. It's from the GRE.
So: r =[(3.49rad/s)(r)]^2/[mu_s(g)] ?

Yep just solve for r. You could have all along used rotational velocity instead of just velocity. So mv^2/r = mrw^2. Also if your studying for the GRE I recommend http://grephysics.net. It is a great site that works out all the problems of the 4 tests which have been released.
 

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