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In defining conservative force, we say that

"The potential energy difference is path independent."

However, as far as I understand, potential energy only exists when there is a force field.

People say one example of non-conservative force.

By definition, non-conservative force should be the one in which the difference in potential energy is path dependent. But where is potential energy for friction which is not a force field?

Qmechanic
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1 Answers1

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I think you mean to say a conservative force $\mathbf F$ is one where we can define a potential energy $U$ such that $$\mathbf F=-\nabla U$$

Then the work done by that force is independent of the path and only depends on the endpoints of the path. In other words, the work is given by: $$W=\int\mathbf F\cdot\text d\mathbf l=\int(-\nabla U)\cdot\text d\mathbf l=U_{\text{start}}-U_{\text{end}}$$ by the fundamental theorem of calculus.

On the other hand, we cannot express a non-conservative force in terms of a potential energy. Therefore, we cannot apply the fundamental theorem of calculus to the work integral, and therefore there is a path dependence on the work.

BioPhysicist
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