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MIT 8.01 Physics I Classical Mechanics, Fall 1999
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Please I need help with a new question, this has a solution that I can't still dig. See the attached JPG
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This is the solution I cant dig. Any help is welcome.
The equations for motion under constant acceleration are: \[v=u+at\] \[s=ut+at ^{2}/2\] In this case u=0. And the question acts for motion ALONG the board. But the given acceleration is vertical. You've to break it into its components, such that one component is along the board. |dw:1333081367432:dw| So the acceleration along the board is a0sintheta. Now just substitute: \[a=a0\sin \theta\]
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