Difference between revisions of "Forest UCM Energy PE n ConsForces"
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: <math>\vec{F} = q \vec v \times \vec B</math> | : <math>\vec{F} = q \vec v \times \vec B</math> | ||
+ | |||
+ | |||
+ | =Potential Energy= | ||
+ | |||
+ | If ALL External forces are conservative | ||
+ | |||
+ | Then a poetential energy U(r) may be defined such that the total energy of the system is constant (conserved) | ||
+ | |||
+ | : <math>E_{tot} = T + U(r) =</math> constant | ||
+ | |||
+ | where | ||
+ | :<math>U(r) \equiv \int_{r_o}^r \vec{F}(r) \cdot d\vec{}r</math> | ||
[[Forest_UCM_Energy#PE_.26_Conservative_Force]] | [[Forest_UCM_Energy#PE_.26_Conservative_Force]] |
Revision as of 11:13, 22 September 2014
Potential Energy and Conservative Forces
Conservative Forces
What is a conservative Force?
Two conditions are neccessary for a Force to be conservative.
- The force on depends on the objects position (F = F(r)). Not on time nor velocity
- The work done by the force in displacing the object between two points is independent of the path taken.
Examples of conservative forces
Examples of Non Conservaive Forces
Potential Energy
If ALL External forces are conservative
Then a poetential energy U(r) may be defined such that the total energy of the system is constant (conserved)
- constant
where