Rotational Motion Problem with Varying Centripetal Force and Friction

In summary, the equation for the number of revolutions of a cylinder with no translational motion is ## \frac{(1+k^2)R (\omega_0)^2}{8 \pi g k(1+k)} ##.
  • #1
Pi-is-3
49
13
Homework Statement
Find the number of revolutions by the cylinder.
Relevant Equations
$$ \tau = I \alpha $$
Change in Kinetic energy = Work done
Hello, I'm stuck in this rotational motion problem (advanced high school level).

20200209_013940.jpg

Source: Problems in General Physics- IE Irodov

My attempt(s):

First I tried using work done by the moment of friction (mgkR) and equated it with change in KE.

I got the answer as ## \frac{R (\omega_0)^2}{8 \pi g k} ##.

However, the correct answer is ## \frac{(1+k^2)R (\omega_0)^2}{8 \pi g k(1+k)} ## .

The first mistake I thought of is not including centripetal, but the centripetal is varying with ## \omega ## and whenever I solve it that way I am not even getting close to the answer. Using ## \tau=I \alpha ## is getting nowhere either.

Any hint is appreciated. Thank you.
 
Physics news on Phys.org
  • #2
Pi-is-3 said:
Homework Statement:: Find the number of revolutions by the cylinder.
Relevant Equations:: $$ \tau = I \alpha $$
Change in Kinetic energy = Work done

Hello, I'm stuck in this rotational motion problem (advanced high school level).

View attachment 256836
Source: Problems in General Physics- IE Irodov

My attempt(s):

First I tried using work done by the moment of friction (mgkR) and equated it with change in KE.

I got the answer as ## \frac{R (\omega_0)^2}{8 \pi g k} ##.

However, the correct answer is ## \frac{(1+k^2)R (\omega_0)^2}{8 \pi g k(1+k)} ## .

The first mistake I thought of is not including centripetal, but the centripetal is varying with ## \omega ## and whenever I solve it that way I am not even getting close to the answer. Using ## \tau=I \alpha ## is getting nowhere either.

Any hint is appreciated. Thank you.
Please post your working (and not as an image).
Did you draw a force diagram? If so please post that as an image, or list the forces involved.
Remember, both surfaces have friction.
 
  • Like
Likes etotheipi
  • #3
You said you tried using work; can you devise an expression relating the number of revolutions to the angular work done by the two frictional forces?
 
  • #4
etotheipi said:
You said you tried using work; can you devise an expression relating the number of revolutions to the angular work done by the two frictional forces?
I think @Pi-is-3's error is in determining those forces.
 
  • Like
Likes Pi-is-3 and etotheipi
  • #5
I am unable to find the frictional force on the left wall.
 
  • #6
Pi-is-3 said:
I am unable to find the frictional force on the left wall.

If you draw a free body diagram of the situation, what equations can you write down involving the normal forces, frictional forces and weight?
 
  • Like
Likes Pi-is-3 and CPW
  • #7
In determining the reaction force on the cylinder by the wall, consider that there is no translational acceleration of the center of mass of the cylinder.
 
  • Like
Likes Pi-is-3
  • #8
15811993452328846205678882829423.jpg


Ignore the minus sign behind mgk. Their has to be some involvement of centripetal force in friction, but I am not sure how, because it is directed towards the center, and not towards the ground. I know I have probably done it very wrong. I'm sorry if it's too bad.
 
  • #9
Oh wait, maybe the normal reaction at ground isn't mg. I have had an idea, let me try it out first.
 
  • Like
Likes etotheipi
  • #10
CPW said:
In determining the reaction force on the cylinder by the wall, consider that there is no translational acceleration of the center of mass of the cylinder.
Got it! Since their is no translational motion, the normal reaction from ground+ frictional on the left wall= mg.

And, friction on ground = Normal reaction from the left wall.

Done!
 
  • #11
Thank you everyone, this problem has been solved.
 

FAQ: Rotational Motion Problem with Varying Centripetal Force and Friction

What is rotational motion?

Rotational motion is the movement of an object around a fixed point or axis. It occurs when an object rotates or spins in a circular motion.

What is the difference between rotational motion and linear motion?

The main difference between rotational motion and linear motion is the type of movement. Rotational motion involves circular movement around a fixed point, while linear motion involves movement in a straight line.

What is the formula for calculating rotational motion?

The formula for calculating rotational motion is angular velocity (ω) = angular displacement (θ) / time (t). This formula is used to calculate the speed at which an object is rotating.

What are some real-life examples of rotational motion?

Some common examples of rotational motion include spinning tops, wheels on a car, and the rotation of the Earth on its axis. Other examples include merry-go-rounds, ceiling fans, and the rotation of a helicopter's rotor blades.

How does rotational motion affect an object's stability?

Rotational motion can affect an object's stability by changing its center of mass. If the center of mass is shifted outside of the base of support, the object may become unstable and fall over. This is why balancing on a tightrope or a unicycle requires precise control of rotational motion.

Back
Top