Conservative and non-conservative forces

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Homework Help Overview

The discussion revolves around the concepts of conservative and non-conservative forces, exploring their definitions and implications in physics. Participants seek clarification on these terms and their applications in energy conservation.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants attempt to define conservative forces as those that conserve total energy, contrasting them with non-conservative forces that do not. Questions arise regarding the nature of potential energy and its dependence on work done by conservative forces.

Discussion Status

Some participants provide examples and explanations of conservative and non-conservative forces, while others question the conventions surrounding potential energy and its definitions. The discussion includes various interpretations of the concepts without reaching a consensus.

Contextual Notes

There is a noted lack of clarity in the original teaching of the topic, prompting participants to seek simpler explanations. The discussion also touches on the conventions used in defining potential energy and the implications of path dependence in non-conservative forces.

JasonAdams
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Can somebody please help me understand conservative and non-conservative forces? My teacher didn't really spend too much time teaching it. Can somebody explain it in the simplest terms possible?
 
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JasonAdams said:
Can somebody please help me understand conservative and non-conservative forces? My teacher didn't really spend too much time teaching it. Can somebody explain it in the simplest terms possible?

http://en.wikipedia.org/wiki/Conservative_force
 
"Conservative" forces conserve the total energy of an object and non-conservative forces don't! That, at any rate, is where the name comes from. Since total energy of an object is the sum of kinetic energy (depending only on speed) and potential energy (depending only on position), if you move an object around with only conservative forces involved, finally returning it to its orignal position and original speed, you have not changed the total energy and so have done no net work. Gravity is an example of a conservative force. The force moving planets around the sun returns then, eventually, to the same point in their orbit with the same speed and so does no net work. That's why gravity doesn't "run out"!

Friction, on the other hand, is a non-conservative force. If you move a refrigerator across the kitchen you are not changing its height and so not its potential energy. If after moving it across the room and leaving it standing still you have not changed its total energy. But you certainly will have to do work! You have to do work to overcome friction- that work goes not into the energy of the refrigerator but causes the floor to be slightly warmer.
 
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In addition, the potential energy can only be defined for the (minus) work of a conservative force. The key is that the work depends ONLY on the starting and ending points, and not on the trajectory. Otherwise (for a non-conservative force) the path has to be specified, so it makes no sense to speak of a potential energy which should depend only on the position.

The path-independence of the work is equivalent to saying that the net work (due to that conservative force) in any closed path is zero.
 
Thanks for the help.
 
xnick said:
In addition, the potential energy can only be defined for the (minus) work of a conservative force.

Isn't that just a convention?
 
neutrino said:
Isn't that just a convention?

I guess the sign is conventional (although i don't think anyone's going to change it now) and also you can add an arbitrary constant to the potential energy and get the same physical results, since the quantities of interest are energy differences.

But the force MUST be conservative.
 
Conservative - point dependent
Non-conservative - path dependent
 

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