Difference between revisions of "Conservative force"
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| − | Conservative [[force | + | '''Conservative [[force]]s''' are those that possess certain properties:<ref>Serway and Beichner, ''Physics for Scientists and Engineers'', Fifth Edition</ref> |
| − | + | * The [[work]] it does on a particle is independent of its [[trajectory]]. | |
| + | * The work done on a particle that moves along a closed trajectory (where the initial and final positions are the same, or d<sub>i</sub> = d<sub>f</sub>) = 0) is zero. | ||
| + | * The force can be written as the negative of the gradient of a potential energy function, i.e. <math>\vec F = - \nabla U </math>. | ||
| + | * The [[curl]] of the force, <math>\vec{F}</math> is zero, <math>\nabla \times \vec{F} = 0</math> | ||
| − | + | When the only forces present in a system are conservative, [[energy]] is conserved. | |
| − | + | Examples of conservative forces include: | |
| − | + | * [[Gravitational force]] | |
| + | * [[Hooke's Law|Force performed by a spring]] | ||
| − | + | [[Friction]] is an example of a non-conservative force: | |
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| − | [[ | ||
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== References == | == References == | ||
| − | + | {{reflist}} | |
| − | + | [[Category:Mechanics]] | |
| − | [[Category: Mechanics]] | ||
Latest revision as of 13:58, April 6, 2017
Conservative forces are those that possess certain properties:[1]
- The work it does on a particle is independent of its trajectory.
- The work done on a particle that moves along a closed trajectory (where the initial and final positions are the same, or di = df) = 0) is zero.
- The force can be written as the negative of the gradient of a potential energy function, i.e. <math>\vec F = - \nabla U </math>.
- The curl of the force, <math>\vec{F}</math> is zero, <math>\nabla \times \vec{F} = 0</math>
When the only forces present in a system are conservative, energy is conserved.
Examples of conservative forces include:
Friction is an example of a non-conservative force:
References
- â Serway and Beichner, Physics for Scientists and Engineers, Fifth Edition