Understanding Friction Between Two Disks: A Problem in Rotational Dynamics

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Homework Help Overview

This discussion revolves around a problem in rotational dynamics involving friction between two disks. Participants are analyzing the application of Newton's laws for rotation and the relationship between torque, moment of inertia, and frictional forces.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the application of Newton's second law for rotation to both disks, questioning the role of moment of inertia and the calculations leading to differing frictional force values.

Discussion Status

The discussion is active, with participants raising questions about the assumptions made in the calculations and the interpretation of forces acting on the disks. Some guidance has been offered regarding the need to consider multiple torques acting on the disks.

Contextual Notes

There is a noted confusion regarding the application of linear versus angular accelerations, as well as the implications of different approaches leading to inconsistent force values.

JD_PM
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Homework Statement



Captura de pantalla (471).png


This problem was originally posted on Physics Problems Q&A: http://physics.qandaexchange.com/?qa=616/friction-between-two-disks

Homework Equations



Second Newton's law for rotation:

$$\tau = I \alpha = RF$$

The Attempt at a Solution



I tried to solve this problem as follows:

Using Second Newton's law for rotation on disk 2R:

$$2Rf = I \alpha = \frac{1}{2} M (2R)^2 \frac{a}{2R} $$

Plugging the numbers into the equation we get:

$$f = 2N$$

OK at this point, now let's do the same on disk R:

$$Rf = I \alpha = \frac{1}{2} M (R)^2 \frac{a}{R} $$

Plugging the numbers into the equation we get:

$$f = 1N$$

So I get different values for ##f## while I have to get the same value! What am I missing on my calculations on disk A?
 

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I don't see why the moment of inertia of A comes into it , or it's radius , or mass...

The force on B is applied at the point of contact , and it's the inertia of B that resists this force.
 
JD_PM said:
OK at this point, now let's do the same on disk R:
There are two torques acting on that disc. Your equation only shows one.
But your problem with this approach is you cannot evaluate the other torque without first finding the frictional force the way you did.
 
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oz93666 said:
I don't see why the moment of inertia of A comes into it , or it's radius , or mass...

The force on B is applied at the point of contact , and it's the inertia of B that resists this force.
JD_PM has already answered correctly the question as posed, but is wondering why a different approach seems to give a different answer.
 
haruspex said:
There are two torques acting on that disc. Your equation only shows one.
But your problem with this approach is you cannot evaluate the other torque without first finding the frictional force the way you did.

Yeah I see what you mean:

$$FR - fR = I \alpha = \frac{1}{2} M (R)^2 \frac{a}{R}$$

$$F - f = 1N$$

So F has to be 3N. (I used the value I got on disk 2R analysis)

But there is a problem: we know the acceleration and the mass of disk R; we can get F (using disk R):

$$F = M a = 1N$$

Mmm so there is something wrong here... F values are different using different approaches
 
JD_PM said:
we know the acceleration and the mass of disk R; we can get F (using disk R):

F=Ma=1N​
I do not understand where this equation comes from. There are no linear accelerations, only angular accelerations.
 
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haruspex said:
I do not understand where this equation comes from. There are no linear accelerations, only angular accelerations.

Yeah, my bad thanks.
 

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