Work: Is Moving an Object Back to Its Original Spot Worth Anything?

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Homework Help Overview

The discussion revolves around the concept of work in physics, specifically whether moving an object back to its original position results in any work being done. Participants are exploring the implications of the work formula and the definitions of work in a physics context.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Some participants attempt to clarify the definition of work, noting that if the net displacement is zero, the work done is also zero. Others introduce the concept of dot products to explain work in terms of force and displacement vectors.
  • Questions arise regarding the assumptions made about the forces acting on the object, with some suggesting that variable forces could lead to different interpretations of work done.
  • One participant proposes breaking down the work into components to analyze the situation further.

Discussion Status

The discussion is ongoing, with various interpretations being explored. Some participants provide insights into the mathematical aspects of work, while others question the assumptions regarding forces. There is no explicit consensus, but several productive lines of reasoning are being examined.

Contextual Notes

Participants are considering different scenarios, including the effects of variable forces and circular motion, which complicate the straightforward application of the work formula. The discussion reflects a range of understanding regarding the physics concepts involved.

BadSkittles
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Hello, if an object is moved to the right and then to the left back to its original spot, is work 0. Or would work still have a value?

Work = Force * Delta x.

It just doesn't seem to make sense to say that there is no work done even when you moved it around.
 
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In physics, work has a much more precise definition than the everyday meaning of work. You seem to be confusing the two definitions. As you can see from the equation in your post, if either the magnitude of the component of the net force parallel to the displacement of the object or the displacement of the object is zero, then the net work done on the object is zero. This result is nothing more than a direct consequence of the definition of work in physics.
 
BadSkittles said:
Hello, if an object is moved to the right and then to the left back to its original spot, is work 0. Or would work still have a value?

Work = Force * Delta x.

It just doesn't seem to make sense to say that there is no work done even when you moved it around.
The equation for work is generally specified as a dot product: ##W = \vec{F} \cdot \vec{Δx}##

If the force that moves your object to the right is also directed to the right, and if the force that moves it back again is directed leftwards in the direction of the motion that returns it to its origin, then in both cases positive work will be done on the object and the total work will be a positive, nonzero value.
 
If you haven't covered dot products yet... What happens if you look at it in two parts...

Work = (work required to move it right) + (work required to move it left)
Work = (+force * +deltaX) + (-force * -deltaX)
= 2 * force * deltaX

The "-" signs are there because the direction of the force and displacement has changed.
 
Is it fair to assume so much about the force(s) acting on the object? It isn't difficult to imagine a case in which variable forces produce the required motion but the net work done on the object is zero.
 
QED Andrew said:
Is it fair to assume so much about the force(s) acting on the object? It isn't difficult to imagine a case in which variable forces produce the required motion but the net work done on the object is zero.

Sure, take circular motion for example. The centripetal force acts always towards the center of the motion and is always at right angles to the direction of motion. Thus there is no component of the force acting along the direction of motion, hence the work done is zero yet the object travels away from and returns to a given location repeatedly.

When more complicated variable forces are involved, the usual approach is to integrate ##\vec{F}\cdot\vec{ds}## over the path the object takes.
 
QED Andrew said:
Is it fair to assume so much about the force(s) acting on the object?

No clearly it's not. I only offered that as a simple explanation of the particular example described by the OP.

Is there a way to explain the general case without reference to dot products?
 

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