Definition of work done by torque

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SUMMARY

The work done by torque can be derived from the equation W = ∫ F ⋅ ds, where ds is expressed as dθ × r. This leads to the formulation W = ∫ Torque ⋅ dθ, establishing a relationship between torque and angular displacement. The direction of dθ is perpendicular to the plane of rotation, aligning with the angular velocity vector. Understanding these relationships is crucial for analyzing rotational dynamics in physics.

PREREQUISITES
  • Understanding of vector calculus and cross products
  • Familiarity with rotational dynamics concepts
  • Knowledge of torque and angular displacement
  • Basic principles of polar coordinates
NEXT STEPS
  • Study the relationship between torque and angular momentum
  • Learn about the applications of the vector triple product in physics
  • Explore the implications of angular velocity in rotational motion
  • Investigate the effects of forces acting at angles on rotational systems
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Physics students, mechanical engineers, and anyone studying rotational dynamics and torque in mechanical systems.

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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