Definition of work done by torque

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Homework Help Overview

The discussion revolves around deriving the work done by torque, specifically through the relationship between torque, force, and angular displacement. The original poster attempts to understand the direction of angular displacement (dθ) in relation to the radius (r) and the force (F) involved in the work done by torque.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between torque and angular displacement, questioning the direction of dθ and its relationship to the radius vector. They discuss the implications of forces acting at angles to the rotation axis and the nature of angular velocity.

Discussion Status

Some participants have provided insights regarding the direction of dθ and its perpendicularity to the plane of circular motion. The discussion is ongoing, with multiple interpretations being explored regarding the relationships between the vectors involved.

Contextual Notes

There is a mention of a specific scenario involving a car skidding, which introduces considerations about forces acting at angles to the rotation axis. This context may influence the assumptions being examined in the discussion.

Cedric Chia
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I' m trying to derive the work done by a torque from W = ∫ F ⋅ ds and I' ve looked up the internet, it said:

W = ∫ F ⋅ ds ( since ds = dθ × r ) ---------------------------------------- ( Line 1 )

it can be written as

W = ∫ F ⋅ dθ x r

this is a vector triple product , thus can also be written as

W = ∫ r × F ⋅ dθ


W = ∫ Torque ⋅ dθ ----------------------------------------------------- ( Line 2 )

My question is :
In what direction is dθ pointing so that when I cross-product dθ and r ( Line 1 ), it become ds ? And also, when I dot-product Torque and dθ ( Line 2 ) , what is the angle between them ?
 
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Cedric Chia said:
I' m trying to derive the work done by a torque from W = ∫ F ⋅ ds and I' ve looked up the internet, it said:

W = ∫ F ⋅ ds ( since ds = dθ × r ) ---------------------------------------- ( Line 1 )

it can be written as

W = ∫ F ⋅ dθ x r

this is a vector triple product , thus can also be written as

W = ∫ r × F ⋅ dθ


W = ∫ Torque ⋅ dθ ----------------------------------------------------- ( Line 2 )

My question is :
In what direction is dθ pointing so that when I cross-product dθ and r ( Line 1 ), it become ds ? And also, when I dot-product Torque and dθ ( Line 2 ) , what is the angle between them ?
A rotation can be represented as a vector along the axis of rotation, so it is normal to the plane of rotation. If the force lies in that plane then it will be parallel to the rotation vector. But in general it need not be. E.g. consider a car skidding at an angle, brakes off. The frictional force wIll be at any angle to the rotation axis.
 
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haruspex said:
A rotation can be represented as a vector along the axis of rotation, so it is normal to the plane of rotation. If the force lies in that plane then it will be parallel to the rotation vector. But in general it need not be. E.g. consider a car skidding at an angle, brakes off. The frictional force wIll be at any angle to the rotation axis.
Thanks for the reply, so the dθ is not in the same direction with the unit vector θ hat ? ( which we introduced in the polar coordinates, θ hat is tangent to the circular motion ) . Instead, dθ is perpendicular to the plane of circular motion ( same direction as angular velocity ) ?
 
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Cedric Chia said:
Instead, dθ is perpendicular to the plane of circular motion ( same direction as angular velocity ) ?
Yes. In fact, ##d\theta/dt## is the angular velocity.
 
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Orodruin said:
Yes. In fact, ##d\theta/dt## is the angular velocity.
Thank you
 

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