Difference between revisions of "Forest UCM Energy Line1D"
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(Created page with " Forest_UCM_Energy#Energy_for_Linear_1-D_systems") |
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+ | The equation of motion for a system restricted to 1-D is readily solved from conservation of energy when the force is conservative. | ||
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+ | : <math>T + U(x) =</math> cosntant <math>\equiv E</math> | ||
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+ | : <math>\Rightarrow T = E - U(x)</math> | ||
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+ | :<math> \frac{1}{2} m \dot {x}^2 = E -U(x)</math> | ||
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+ | : <math>dot x = \pm \sqrt{\frac{2\left (E-U(x) \right )}{m}}</math> | ||
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[[Forest_UCM_Energy#Energy_for_Linear_1-D_systems]] | [[Forest_UCM_Energy#Energy_for_Linear_1-D_systems]] |
Revision as of 12:07, 26 September 2014
The equation of motion for a system restricted to 1-D is readily solved from conservation of energy when the force is conservative.
- cosntant