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course_planning:183_projects:f17_project_15_solution [2017/12/07 00:04] – pawlakal | course_planning:183_projects:f17_project_15_solution [2017/12/07 00:48] (current) – pawlakal | ||
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w=7.42rad/s | w=7.42rad/s | ||
- | We can use v=rw to convert this to the linear speed that the steel ball leaves the catapult | + | We can use $v=rw$ to convert this to the linear speed that the steel ball leaves the catapult |
- | $$v_{i, steel}=(7.42 rad/s)*(4 m)$$ | + | $$v_{i, steel}=(4 m)*(7.42 rad/s)$$ |
- | vi,steel=29.68 | + | $$v_{i, steel}=29.68 |
- | Now we use energy conservation and linear momentum conservation to consider the collision between the steel ball and the shark. We take our system to be the shark and steel ball, and we assume that the shark starts at rest. For momentum conservation, | + | Now we use energy conservation and linear momentum conservation to consider the collision between the steel ball and the shark. We take our system to be the shark and steel ball, and we assume that the shark starts at rest. We also assume that the collision is elastic. For momentum conservation, |
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For energy conservation, | For energy conservation, | ||
- | $$/frac{1}{2}m_{steel}v_{i, | + | $$KE_{i, steel}+KE_{i, |
+ | $$\frac{1}{2}m_{steel}v_{i, | ||
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+ | Students will need to look up a mass for a shark. Using 900 kg, solving this system of equations for the final velocities of the steel ball and shark, we get: | ||
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+ | vf,steel=−29.03m/s | ||
+ | vshark=0.65m/s | ||
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+ | So, the shark doesn' | ||
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+ | <WRAP tip> | ||
+ | ==Tutor Questions: | ||
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+ | * **Question: | ||
+ | * **Expected Answer: | ||
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+ | * **Question: | ||
+ | * **Expected Answer: | ||
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+ | * **Question: | ||
+ | * **Expected Answer: | ||
+ | </ |