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| 183_notes:examples:a_yo-yo [2014/11/06 02:41] – pwirving | 183_notes:examples:a_yo-yo [2014/11/06 02:59] (current) – pwirving | ||
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| ΔKtrans = ∫fi→Fnet⋅d→rcm | ΔKtrans = ∫fi→Fnet⋅d→rcm | ||
| + | |||
| + | ΔEsys = Wsurr | ||
| === Solution === | === Solution === | ||
| Line 68: | Line 70: | ||
| a: | a: | ||
| - | From the Energy Principle (point particle only has Ktrans): | + | From the Energy Principle ( when dealing with a point particle |
| + | |||
| + | ΔKtrans = ∫fi→Fnet⋅d→rcm | ||
| + | |||
| + | Substituting in for the forces acting on the yo-yo for Fnet and the change in position in the y direction for the centre of mass for d→rcm we get: | ||
| ΔKtrans=(F−mg)ΔyCM | ΔKtrans=(F−mg)ΔyCM | ||
| - | ΔyCM=−h(fromdigram) | + | As indicated in diagram in the b section of the representation: |
| - | ΔKtrans=(F−mg)(−h)=(mg−F)h | + | ΔyCM=−h |
| + | |||
| + | Substitute in −h for yCM | ||
| + | |||
| + | $\Delta K_{trans} = (F - mg)(-h)$ | ||
| + | |||
| + | Multiply across by a minus and you get an equation for ΔKtrans that looks like: | ||
| + | |||
| + | $\Delta K_{trans} | ||
| b: | b: | ||
| + | |||
| + | From the energy principle we know: | ||
| + | |||
| + | ΔEsys = Wsurr | ||
| + | |||
| + | In this case we know that the change in energy in the system is due to the work done by the hand and the work done by the Earth. | ||
| ΔEsys=Whand+WEarth | ΔEsys=Whand+WEarth | ||
| + | |||
| + | Because we are dealing with the real system in this scenario the change in energy is equal to the change in translational kinetic energy + the change in rotational kinetic energy. | ||
| + | |||
| + | ΔKtrans+ΔKrot=Whand+WEarth | ||
| + | |||
| + | Substitute in the work represented by force by distance for both the hand and the Earth. | ||
| ΔKtrans+ΔKrot=Fd+(−mg)(−h) | ΔKtrans+ΔKrot=Fd+(−mg)(−h) | ||
| - | ΔKtrans=(mg−F)h (From part (a)) | + | From part (a) of the problem we can substitute in (mg−F)h for ΔKtrans as the translational kinetic energy will be the same. |
| + | |||
| + | ΔKtrans=(mg−F)h | ||
| + | |||
| + | Substituting this into our equation leaves us with: | ||
| (mg−F)h+ΔKrot=Fd+mgh | (mg−F)h+ΔKrot=Fd+mgh | ||
| + | |||
| + | Solve for change in rotational kinetic energy: | ||
| ΔKrot=F(d+h) | ΔKrot=F(d+h) | ||