Understanding Work in Physics: Force and Displacement Relationship

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Discussion Overview

The discussion centers around the concept of work in physics, specifically the relationship between force and displacement. Participants explore different interpretations of how work is calculated, particularly in the context of external forces and conservative forces.

Discussion Character

  • Debate/contested

Main Points Raised

  • One participant asserts that work done by a force is the scalar product of the force vector and the potential displacement vector, while another claims it should be based on the actual displacement regardless of other forces.
  • There is a contention regarding the calculation of work done by gravity, with one participant suggesting it could vary based on external forces, while another insists it is always calculated as mg(y_1 - y_2).
  • A later reply acknowledges the relevance of conservative forces in this context.

Areas of Agreement / Disagreement

Participants express differing views on the definition and calculation of work, indicating that multiple competing interpretations remain unresolved.

Contextual Notes

Participants highlight the dependence on definitions of displacement and the implications of external forces on work calculations, but do not resolve these issues.

Vykan12
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I've always thought that the work done by a force is the scalar product of the force vector and the potential displacement vector it would have if no other forces were acting on it. My teacher says that it is really the product of the force vector and the resultant displacement regardless of what other forces act on the system, and that you'd get the same net work with either calculation.

I don't see how the way he defines it would make any sense. For example, if you derive the work done by gravity, you could find it to be just about anything depending on the external forces in question, rather than just mg(y_1 - y_2). So what is the true convention?
 
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Hi Vykan12! :smile:

Work done by a particular force is (integral of) that force times the actual displacement (of the point of application of the force, if it's not a point body).

What the displacement would be if there were no other forces is irrelevant. :wink:
 
Vykan12 said:
For example, if you derive the work done by gravity, you could find it to be just about anything depending on the external forces in question, rather than just mg(y_1 - y_2).
No, regardless of the path the object takes the work done by gravity will always be mg(y_1 - y_2).
 
I can see that's where the properties of conservative forces come into play. Interesting.
 

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