Finding moment of inertia of a pulley

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Homework Help Overview

The problem involves two masses, m1 = 3 kg and m2 = 4 kg, hanging from opposite sides of a pulley with a radius of 0.15 m. The heavier mass falls 0.34 m in 4 seconds after being released from rest, and the task is to find the rotational inertia of the pulley.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss applying Newton's second law to each mass and the relationship between linear and angular acceleration. There are attempts to derive tensions in the rope and relate them to the torque on the pulley.

Discussion Status

Some participants provide insights into the relationship between tensions and the resulting torque, while others express confusion about the implications of the tensions on the system's motion. There is an ongoing exploration of the correct interpretation of the forces at play.

Contextual Notes

Participants are navigating through the implications of Newton's laws and the setup of the problem, with some questioning assumptions about the directions of forces and the resulting motion of the masses.

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Homework Statement


Two masses, one of m_{1}= 3kg, the other of m_{2}=4kg, hang from opposite sides of a pulley of radius .15m. When released from rest, the heavier mass falls .34m in 4s. What is the rotational inertia of the pulley?


Homework Equations


Newton's second law and \tau = I\alpha

The Attempt at a Solution


I tried using Newton's 2nd law on each of the masses:
T_{1} - m_{1}g = m_{1}a
m_{2}g - T_{2} = m_{1}a
where T_{1} and T_{2} are the tensions of the rope on each mass.
solving for these tensions yields
T_{1} = m_{1}(g+a)
T_{2} = m_{2}(g-a)
I originally planned to plug these into \tau = I\alpha and use linear kinematics equations to solve for the acceleration and therefore the angular acceleration, but it is clear that T_{1} is greater than T_{2} something seems to have gone wrong, because wouldn't this imply that, through Newton's third law, the net torque would be causing m_{1}, the lighter block, to fall? Thanks for the help.
 
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My approach would be:
Find the acceleration of the block and relate this to the angular acceleration of the pulley then find the resultant torque on the pulley. You don't need to worry about tensions.
 
But don't the tensions determine the resultant torque on the pulley?
 
Edit: Yeah sorry I'm talking rubbish, I'll have another think tomorrow
 
Last edited:
bologna121121 said:

Homework Statement


Two masses, one of m_{1}= 3kg, the other of m_{2}=4kg, hang from opposite sides of a pulley of radius .15m. When released from rest, the heavier mass falls .34m in 4s. What is the rotational inertia of the pulley?

Homework Equations


Newton's second law and \tau = I\alpha

The Attempt at a Solution


I tried using Newton's 2nd law on each of the masses:
T_{1} - m_{1}g = m_{1}a
m_{2}g - T_{2} = m_{1}a
where T_{1} and T_{2} are the tensions of the rope on each mass.
solving for these tensions yields
T_{1} = m_{1}(g+a)
T_{2} = m_{2}(g-a)
I originally planned to plug these into \tau = I\alpha and use linear kinematics equations to solve for the acceleration and therefore the angular acceleration, but it is clear that T_{1} is greater than T_{2} something seems to have gone wrong, because wouldn't this imply that, through Newton's third law, the net torque would be causing m_{1}, the lighter block, to fall? Thanks for the help.

Actually, you're doing okay. T1 will be less that T2 because the mass multipliers make a difference.

You can determine the acceleration form the given information: "the heavier mass falls .34m in 4s".

Once you have the acceleration you can determine the tensions T1 and T2. You'll only need the equation for the motion of the pulley to complete.
 
Last edited:
bologna121121 said:

Homework Statement


Two masses, one of m_{1}= 3kg, the other of m_{2}=4kg, hang from opposite sides of a pulley of radius .15m. When released from rest, the heavier mass falls .34m in 4s. What is the rotational inertia of the pulley?

Homework Equations


Newton's second law and \tau = I\alpha

The Attempt at a Solution


I tried using Newton's 2nd law on each of the masses:
T_{1} - m_{1}g = m_{1}a
m_{2}g - T_{2} = m_{1}a
where T_{1} and T_{2} are the tensions of the rope on each mass.
solving for these tensions yields
T_{1} = m_{1}(g+a)
T_{2} = m_{2}(g-a)
I originally planned to plug these into \tau = I\alpha and use linear kinematics equations to solve for the acceleration and therefore the angular acceleration, but it is clear that T_{1} is greater than T_{2} something seems to have gone wrong, because wouldn't this imply that, through Newton's third law, the net torque would be causing m_{1}, the lighter block, to fall? Thanks for the help.

you are forgotting what T1 and T2 are actually doing..

T1 > T2

that part is clear. but...

T1 is increase net acc of the system by pulling m1 upwards.
T2 is decrease net acc of the system...aka...slowing down m2...by pulling it upwards.

So when T1 > T2 that means the system rotates in the direction of m2. the larger mass.

I hope that clears it up for you.
 
Last edited:
gneill said:
Actually, you're doing okay. T1 will be less that T2 because the mass multipliers make a difference.

You can determine the acceleration form the given information: "the heavier mass falls .34m in 4s".

Once you have the acceleration you can determine the tensions T1 and T2. You'll only need the equation for the motion of the pulley to complete.

that is kinda wrong.

T1>T2

think of it like this.

T2 is a force caused by m1g on m2
T1 is a force caused by m2g on m1
 
Genoseeker said:
that is kinda wrong.

T1>T2

think of it like this.

T2 is a force caused by m1g on m2
T1 is a force caused by m2g on m1

If T1 were greater than T2, then the pulley would turn towards the T1 side and m2 would rise, not fall.
 
bologna121121 said:
T_{1} = m_{1}(g+a)
T_{2} = m_{2}(g-a)
I originally planned to plug these into \tau = I\alpha and use linear kinematics equations to solve for the acceleration and therefore the angular acceleration, but it is clear that T_{1} is greater than T_{2} something seems to have gone wrong, because wouldn't this imply that, through Newton's third law, the net torque would be causing m_{1}, the lighter block, to fall? Thanks for the help.


T1 is not greater than T2.

T2-T1= m2g -m2a -m1g-m1a=g(m2-m1)-a(m2-m1)>0
 
  • #10
bologna121121 said:
T_{1} = m_{1}(g+a)
T_{2} = m_{2}(g-a)
I originally planned to plug these into \tau = I\alpha and use linear kinematics equations to solve for the acceleration and therefore the angular acceleration, but it is clear that T_{1} is greater than T_{2} something seems to have gone wrong, because wouldn't this imply that, through Newton's third law, the net torque would be causing m_{1}, the lighter block, to fall? Thanks for the help.


T1 is no greater than T2.

T2-T1= m2g -m2a -m1g-m1a=g(m2-m1)-a(m2+m1)>0
 

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