Difference between revisions of "Forest UCM Energy 1DCurve"
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The equations of motion for some systems can be reduced to a 1-D description. | The equations of motion for some systems can be reduced to a 1-D description. | ||
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One common system is the atwood machine | One common system is the atwood machine | ||
| + | A solution to two such Atwood machine configurations using Newton's laws is shown below | ||
| + | [[Forest_UCM_NLM_AtwoodMachine]] | ||
[[Forest_UCM_Energy#Energy_for_Curvilinear_1-D_systems]] | [[Forest_UCM_Energy#Energy_for_Curvilinear_1-D_systems]] | ||
Revision as of 18:17, 26 September 2014
The equations of motion for some systems can be reduced to a 1-D description.
One common system is the atwood machine
A solution to two such Atwood machine configurations using Newton's laws is shown below