Difference between revisions of "Forest UCM Energy 1DCurve"
Jump to navigation
Jump to search
| (One intermediate revision by the same user not shown) | |||
| Line 1: | Line 1: | ||
| + | The equations of motion for some systems can be reduced to a 1-D description. | ||
| − | + | ||
| + | do problems 4.30 ,4.31, and 4.34 in class | ||
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]] | ||
Latest revision as of 21:13, 26 September 2014
The equations of motion for some systems can be reduced to a 1-D description.
do problems 4.30 ,4.31, and 4.34 in class
One common system is the atwood machine
A solution to two such Atwood machine configurations using Newton's laws is shown below