Understanding Friction Between Two Disks: A Problem in Rotational Dynamics

AI Thread Summary
The discussion revolves around a problem involving friction between two disks in rotational dynamics. Participants analyze the application of Newton's second law for rotation to determine the frictional force acting on each disk. Discrepancies arise when calculating the frictional force, leading to different values for the force on each disk. The conversation highlights the need to consider multiple torques and the relationship between linear and angular accelerations in the analysis. Ultimately, confusion persists regarding the application of linear force equations in a rotational context.
JD_PM
Messages
1,125
Reaction score
156

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?
 

Attachments

  • Captura de pantalla (471).png
    Captura de pantalla (471).png
    16.1 KB · Views: 755
Physics news on Phys.org
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.
 
  • Like
Likes JD_PM
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.
 
  • Like
Likes JD_PM
haruspex said:
I do not understand where this equation comes from. There are no linear accelerations, only angular accelerations.

Yeah, my bad thanks.
 
Back
Top