Why elementary work is not an exact differential?

Click For Summary

Discussion Overview

The discussion revolves around the nature of elementary work in physics, specifically why it is defined as δW=Fdr rather than as an exact differential dW=Fdr. Participants explore the implications of conservative versus non-conservative forces on the definition of work, and the relationship between work and potential energy.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants note that elementary work is only an exact differential in the case of conservative forces, where work can be related to potential energy.
  • It is argued that work is a line integral that depends on the path taken, which means that δW is not an exact differential by definition.
  • One participant emphasizes that writing work as an exact differential implies that force can be expressed as the derivative of some function of spatial coordinates.
  • Another participant points out that if work were an exact differential, it would suggest that work is a function of state, which contradicts the nature of work as a process that occurs between states.
  • There is a discussion about whether force can be the derivative of a function of spatial coordinates, with references to conservative and non-conservative forces.

Areas of Agreement / Disagreement

Participants express differing views on the implications of work being an exact differential, with some agreeing that it is not applicable in non-conservative scenarios, while others explore the conditions under which work can be considered an exact differential. The discussion remains unresolved regarding the broader implications of these definitions.

Contextual Notes

Participants reference specific equations and concepts from the "Fundamental Laws of Mechanics" by IE Irodov, indicating that their arguments may depend on interpretations of these texts.

phydev
Messages
20
Reaction score
0
Why elementary work is defined as δW=Fdr?
My ques. is not on the definition; it is on why it cannot be dW=Fdr?
 
Physics news on Phys.org
It is only an exact differential int he case of a conservative force. Precisely, if there is a potential we write

dU = -Fdr

which implies that F = -dU/dr.
 
tommyli said:
It is only an exact differential int he case of a conservative force. Precisely, if there is a potential we write

dU = -Fdr

which implies that F = -dU/dr.

I'm not talking about U(potential energy function), I'm asking about W.
I know that in case of conservative/potential field δW=-dU.

Reference: Fundamental Laws of Mechanics, IE irodov
from equation 3.1 to 3.49
wherever needed he used δA for elementary work, in general!
 
Work is a line integral:

W=\oint \mathbf F \cdot d\mathbf r

It is path independent in the case of a conservative force, but in general the integral depends on the path. In other words, \mathbf F \cdot d\mathbf r is not an exact differential by definition (an exact differential is path independent).
 
D H said:
Work is a line integral:

W=\oint \mathbf F \cdot d\mathbf r

It is path independent in the case of a conservative force, but in general the integral depends on the path. In other words, \mathbf F \cdot d\mathbf r is not an exact differential by definition (an exact differential is path independent).

Thanks, it was helpful!
 
phydev said:
I'm not talking about U(potential energy function), I'm asking about W.
I know that in case of conservative/potential field δW=-dU.

Reference: Fundamental Laws of Mechanics, IE irodov
from equation 3.1 to 3.49
wherever needed he used δA for elementary work, in general!

Whenever you write df it implies that the differential operator is applied to the function f, so if you write work as an exact differentail dW implicitly you are saying force can be written as the derivative of some function of spatial coordinates.
 
tommyli said:
Whenever you write df it implies that the differential operator is applied to the function f, so if you write work as an exact differentail dW implicitly you are saying force can be written as the derivative of some function of spatial coordinates.

Yeah! right!
Now, what does it further imply?
Cannot force be derivative of a function of spatial coordinates?

I think I have got it, but request you to elaborate so that I may confirm.

Thanks!
 
If work was an exact differential, for any two points a and b, you could write that the work to go from one point is F(b) - F(a), where F' is work. But this is most certainly not true, as this is saying work is a function of state, i.e. if you have a point, you'd have a work associated to it. This is false, as work is something you use to go from one state to another. It's pretty much like heat. Heat is also not a function of state and depends on the path.
 
phydev said:
Yeah! right!
Now, what does it further imply?
Cannot force be derivative of a function of spatial coordinates?

I think I have got it, but request you to elaborate so that I may confirm.

Thanks!

If force is a derivative of some function of spatial coordinates, this function is called the potential energy, and the force is conservative. Non-conservative forces are certainly not derivatives of any function.
 
  • #10
tommyli said:
If force is a derivative of some function of spatial coordinates, this function is called the potential energy, and the force is conservative. Non-conservative forces are certainly not derivatives of any function.

well... thanks,
I concluded the same!
 

Similar threads

  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 21 ·
Replies
21
Views
3K
  • · Replies 61 ·
3
Replies
61
Views
7K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 48 ·
2
Replies
48
Views
3K
  • · Replies 22 ·
Replies
22
Views
1K
  • · Replies 48 ·
2
Replies
48
Views
6K
  • · Replies 4 ·
Replies
4
Views
6K
  • · Replies 22 ·
Replies
22
Views
2K