Work Energy Method for Rotational Motion

Click For Summary

Homework Help Overview

The discussion revolves around the work-energy method in the context of rotational motion, specifically addressing the work done by frictional forces and the relationship between linear and rotational motion in a system involving a falling mass and a rotating drum.

Discussion Character

  • Conceptual clarification, Assumption checking, Mixed

Approaches and Questions Raised

  • Participants explore the relationship between linear and rotational motion, questioning how both types of motion contribute to the work done in the system. They discuss the use of tension and frictional force in calculating torque and work, raising questions about the definitions and applications of these concepts in different contexts.

Discussion Status

Participants are actively engaging with the problem, seeking clarification on the roles of different forces and how they relate to the work-energy method. Some have provided insights into the distinctions between torque due to tension and friction, while others are confirming their understanding of the concepts involved.

Contextual Notes

There are references to specific diagrams and parts of the problem that may not be fully detailed in the discussion, leading to some confusion about the application of concepts across different contexts. Participants are navigating these complexities without a clear consensus on all points raised.

freshbox
Messages
290
Reaction score
0

Homework Statement



Reference to part C of the question, I would like to ask for work done U1to2, how come linear motion is not included? I thought both linear and rotational exist since the parcel "move downwards" (linear) and the wheel is rotating (rotational)
Thanks...
 

Attachments

  • e1.jpg
    e1.jpg
    52.5 KB · Views: 552
  • e2.jpg
    e2.jpg
    28.5 KB · Views: 578
Last edited:
Physics news on Phys.org
Part C asks for the work on the drum. Why worry about the falling mass? They want you to calculate the work directly.
 
Oh you you are right, sorry didn't read the question clearly :redface:

Just to confirm if they ask me to find the work of frictional force, Fr on the drum and falling mass between position 1 and 2 both linear and rotational will exist correct?

With regards to part c again, To find Torque τ, I know that τ=Tension X Radius so comparing diagram 1 (left) against diagram 2 (right) which i drew a red line to indicate Tension.

How come in the Work Done equation it uses the Frictional Force X Radius and not Tension X radius?Thanks...
 

Attachments

  • c1.jpg
    c1.jpg
    12.7 KB · Views: 563
  • c2.jpg
    c2.jpg
    18.8 KB · Views: 472
freshbox said:
Just to confirm if they ask me to find the work of frictional force, Fr on the drum and falling mass between position 1 and 2 both linear and rotational will exist correct?
If the mass falls and the drum rotates, sure there will be both linear and rotational motion and kinetic energy.
With regards to part c again, To find Torque τ, I know that τ=Tension X Radius so comparing diagram 1 (left) against diagram 2 (right) which i drew a red line to indicate Tension.
Realize that those diagrams refer to different problems.
How come in the Work Done equation it uses the Frictional Force X Radius and not Tension X radius?
Part c asks you for the work done by the frictional force, not the tension.
 
My lecturer told me that τ = tension X radius this concept on the chapter of Kinetics of rotational motion diagram 1 (left)

But he never mention this on the chapter of Work Energy method for rotational motion diagram 2 (right). However, I thought they have the same meaning since both are τ in both formula.
So are you trying to say U1-2=τ X δ
The τ in the equation is actually the frictional force?

And can I say that Torque in τ=Iα and U1-2=τ X δ are actually both different thing?
 

Attachments

  • ex1.jpg
    ex1.jpg
    37.4 KB · Views: 535
  • ex2.jpg
    ex2.jpg
    29.5 KB · Views: 620
freshbox said:
My lecturer told me that τ = tension X radius this concept on the chapter of Kinetics of rotational motion diagram 1 (left)

But he never mention this on the chapter of Work Energy method for rotational motion diagram 2 (right). However, I thought they have the same meaning since both are τ in both formula.
You can calculate the torque due to any force. If the force is tangential to the wheel, then τ = Force X radius. Depending upon the particular problem, that force can be a tension force or a friction force.
So are you trying to say U1-2=τ X δ
The τ in the equation is actually the frictional force?
Right. The torque in that equation is due to the friction force. You are asked to find the work done by the friction force, so you'd use the torque created by that force to calculate the work.
And can I say that Torque in τ=Iα and U1-2=τ X δ are actually both different thing?
Yes, those are different things. The first equation is just Newton's 2nd law as applied to rotation; the torque in that formula should really be the net torque: Ʃτ=Iα.

The second equation is an expression for the work done by some torque. In your problem, it's the work done by the frictional force, which is non-conservative work that will decrease the total mechanical energy of the system.
 
Thank you sir for the clarification.
 

Similar threads

Replies
4
Views
1K
Replies
9
Views
3K
Replies
1
Views
2K
Replies
7
Views
3K
Replies
1
Views
2K
  • · Replies 12 ·
Replies
12
Views
3K
Replies
6
Views
3K
  • · Replies 6 ·
Replies
6
Views
2K
Replies
29
Views
3K