Rotational Mechanics Problem again

In summary, the problem involves a block and a ring connected horizontally, with the formula T = Iα being used to calculate the torque when the block is horizontal. The correct answer is g/3r, but the formula used in the problem is g/2r. To solve this, the torque due to friction force needs to be taken into account, as well as the moment of inertia for the ring. Taking the torque about the center of mass of the ring and using F=ma=mrα for the center of mass of the ring, the correct answer is g/r. However, using the instantaneous axis of rotation may provide an easier solution. The given answer of g/3r may not be correct.
  • #1
thunderhadron
141
0
Hi friends the problem states like this:

https://fbcdn-sphotos-f-a.akamaihd.net/hphotos-ak-ash3/s480x480/68815_2639239357533_424911713_n.jpg

When the attached block is horizontal it is applying torque on the ring. Here I am using the formula T = Iα

So,

mg. r = (mr2(ring) + mr2(block))α

so α = g/2r

But it is not the correct answer. The correct answer is g/3r.

Please help me friends. Thank you in advance.
 
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  • #2
You need to take the torque due to friction force too.

And check your moment of inertia for ring.
 
  • #3
hey, man! What values have you used for the mass of the block and the mass of the ring?
 
  • #4
BruceW said:
hey, man! What values have you used for the mass of the block and the mass of the ring?

Sorry Bruce It happened by mistake.

Taking mass of the ring as 3m the ans is g/4R.
 
  • #5
Pranav-Arora said:
You need to take the torque due to friction force too.

And check your moment of inertia for ring.


Hi Pranav.

But here μ is also absent. Now about which axis I should take torque ? Because If I am taking it about the central axis μ is also there.
 
  • #6
thunderhadron said:
Hi Pranav.

But here μ is also absent. Now about which axis I should take torque ? Because If I am taking it about the central axis μ is also there.

The body rolls without slipping/sliding implies that there is force due to friction too.

You have to take the torque about the CM of ring.
 
  • #7
thunderhadron said:
Hi Pranav.

But here μ is also absent. Now about which axis I should take torque ? Because If I am taking it about the central axis μ is also there.

It is static friction, which needs to be enough to prevent the bottom point of the ring from sliding. No need to know μ.

ehild
 
  • #8
ehild said:
It is static friction, which needs to be enough to prevent the bottom point of the ring from sliding. No need to know μ.

ehild

SO what should I do after that. What should I apply to solve it Not getting exactly. Please Help.
 
  • #9
Pranav-Arora said:
The body rolls without slipping/sliding implies that there is force due to friction too.

You have to take the torque about the CM of ring.

Takinf torque about com,

mg.r + μ. mg r = (mr2 + 3m r2). α

now sticking with μ
 
  • #10
thunderhadron said:
Takinf torque about com,

mg.r + μ. mg r = (mr2 + 3m r2). α

now sticking with μ

Now make an equation for the translational motion.
 
  • #11
Pranav-Arora said:
Now make an equation for the translational motion.

Well I did some wrong in the previous equation,

Right one -

mgr + μ. 4mgr = (mr2 + 3mr2) α

i.e.
g + 4g. μ = 4r.α

For translational motion,

4μ mg = 3ma = 3 mrα

Solving both equations,

α = g/r

Please tell me what i am doing wrong now.
Thank you in advance.
 
  • #12
hi thunderhadron! :smile:

don't forget that the total centre of mass is moving downward, and the total moment of inertia is changing!

you'll probably need to consider the ring and the mass separately :wink:
 
  • #13
thunderhadron said:
Well I did some wrong in the previous equation,

Right one -

mgr + μ. 4mgr = (mr2 + 3mr2) α

i.e.
g + 4g. μ = 4r.α

For translational motion,

4μ mg = 3ma = 3 mrα

Solving both equations,

α = g/r

Please tell me what i am doing wrong now.
Thank you in advance.

I should have been a bit more clear in my previous post. You don't know the frictional force here, so instead of μ. 4mgr, write fr where f is the frictional force.

For translational motion, f=ma=mrα (since its given that it rolls without slipping).

Solve the two equations.
 
  • #14
This time it is easier to use the instantaneous axis.

Apply the parallel axis theorem to get the moment of inertia of the ring with respect to that axis, and add the moment of inertia of the small block. ehild
 
  • #15
So as per you guys instructions I am doing it with full consciousness.

Taking τ = Iα about the center of mass of the ring,

mg.r + f.r = (3mr2 + mr2

takinking F = ma for the com of the ring,

f = 3m.a = 3mr.α

solving both the equations I get the result,
α= g/r.

Which is not correct. That means still doing some wrong here. Please help.
 
  • #16
What can be the direction of the force of friction? Think: when the ring rolls clockwise, the centre accelerates to the right. It is only friction that accelerates the ring and block to the right.

The force of friction accelerates the whole system, ring and block. That is 4m.

And I think the given answer (g/3r) is not correct.

ehild
 
Last edited:
  • #17
I second echild's recommendation of using the instantaneous axis of rotation!
 
  • #18
TSny said:
I second echild's recommendation of using the instantaneous axis of rotation!

Anyway, I do not get the given result. Do you?

ehild
 
  • #19
ehild said:
Anyway, I do not get the given result. Do you?

ehild

Me either. But I do get one of the other choices.
 
  • #20
TSny said:
I second echild's recommendation of using the instantaneous axis of rotation!

thirded! :smile:

(and i too don't get the given answer)
 
  • #21
TSny said:
Me either. But I do get one of the other choices.
Just like me :smile:

ehild
 

1. What is rotational mechanics?

Rotational mechanics is a branch of physics that deals with the motion and forces of objects that are rotating or moving in a circular path. This includes analyzing the relationship between torque, angular velocity, and angular acceleration.

2. What is a rotational mechanics problem?

A rotational mechanics problem is a physics problem that involves applying the principles of rotational motion to solve for unknown quantities, such as the angular velocity, torque, or moment of inertia of a rotating object.

3. How do you approach a rotational mechanics problem?

The first step in solving a rotational mechanics problem is to identify the known and unknown quantities. Then, apply the relevant equations and principles, such as Newton's Second Law for rotational motion or the conservation of angular momentum, to solve for the unknown quantity.

4. What are some common applications of rotational mechanics?

Rotational mechanics has many applications in real-world scenarios, such as in the design of car engines, wind turbines, and amusement park rides. It is also important in understanding the motion of celestial bodies, such as planets and stars.

5. What are some common challenges when solving rotational mechanics problems?

One of the main challenges in solving rotational mechanics problems is visualizing the motion of objects in a circular path and understanding the relationship between linear and angular quantities. It can also be challenging to correctly identify the direction of angular velocity and torque, which can affect the accuracy of the solution.

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