Coefficient of kinetic friction on ramp

Click For Summary
SUMMARY

The coefficient of kinetic friction (μk) required for a block and a disk of equal mass to reach the bottom of a 30° incline simultaneously is derived as μk = (1/3)tan(30°) = 0.192. The derivation involves equating the accelerations of both objects, where the disk's acceleration is a_disk = (2/3)g sin(30°) and the block's acceleration is a_block = g(sin(30°) - μk cos(30°)). The relationship between the two accelerations leads to the final expression for μk.

PREREQUISITES
  • Understanding of Newton's second law of motion
  • Familiarity with rotational dynamics and moment of inertia
  • Knowledge of trigonometric functions, specifically tangent
  • Basic concepts of friction, particularly kinetic friction
NEXT STEPS
  • Study the derivation of the moment of inertia using the parallel axis theorem
  • Explore the relationship between linear and angular acceleration in rolling motion
  • Learn about the effects of friction in different types of motion (translational vs. rotational)
  • Investigate the application of torque in rotational dynamics problems
USEFUL FOR

Physics students, mechanical engineers, and anyone interested in understanding the dynamics of rolling and sliding objects on inclined planes.

UrbanXrisis
Messages
1,192
Reaction score
1
A block and disk with equal masses are released from the same height on a 30° incline. The block slides down the ramp while the disk rolls. If they both reach the bottom at the same time, what must be the coefficient of kinetic (sliding) friction?


ANSWER: mk = (1/3)tanX = (1/3)tan(30°) = 0.192

my question is... how did they derive the equation:
mk = (1/3)tanX

all I got was 2/3 g sin X

\mu m g cos\theta=ma
\mu m g cos\theta=m*\frac{2}{3} g sin\theta
\mu=\frac{2}{3}tan \theta
 
Physics news on Phys.org
UrbanXrisis said:
A block and disk with equal masses are released from the same height on a 30° incline. The block slides down the ramp while the disk rolls. If they both reach the bottom at the same time, what must be the coefficient of kinetic (sliding) friction? ...

\mu m g cos\theta=ma
\mu m g cos\theta=m*\frac{2}{3} g sin\theta
\mu=\frac{2}{3}tan \theta
If they reach the bottom at the same time, then:

t_{block} = \sqrt{2s/a_{block}} = t_{disk} = \sqrt{2s/a_{disk}} so the two accelerations must be equal.

The acceleration of the centre of mass of the disk is given by:

\tau = I\alpha = \frac{3}{2}mr^2a_{disk}/r = mgsin(30)r

This is the tricky part. You have to use the parallel axis theorem to get the moment of inertia about a point on the rim: I_{rim} = I_{cm} + mr^2

So:
(1)a_{disk} = \frac{2}{3}gsin(30)

For the block:

F = ma_{block} = mgsin(30) - \mu_kmgcos(30)

(2)a_{block} = g(sin(30) - \mu_kcos(30))

From (1) and (2):

sin(30)(1 - \frac{2}{3})= \mu_kcos(30)

\mu_k = \frac{1}{3}tan(30)

AM
 
Last edited:
I suppose you have this figured out already but still...

For the disk, it is not really necessary to refer to the rim. If you do so however, you will take the torque contribution from mgsin\theta only and not from the friction force. So I guess for this problem, Andrew's method is better. You can also set up the torque equation about the mass center of the disk, taking torque due to friction only. But you would have to solve another equation (in particular, for translation of the mass center) to eliminate the frictional force. Remember, frictional force is in general not written as a function of the friction coefficients in case of general plane motion (ie rotation + translation) and definitely not in case of rolling. But for the block which does not rotate, frictional force is written as a function of the coefficient of kinetic friction.

Cheers
Vivek
 

Similar threads

  • · Replies 7 ·
Replies
7
Views
1K
  • · Replies 4 ·
Replies
4
Views
3K
Replies
4
Views
3K
  • · Replies 3 ·
Replies
3
Views
1K
Replies
46
Views
5K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 11 ·
Replies
11
Views
1K
Replies
18
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K