183_notes:examples:a_yo-yo

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183_notes:examples:a_yo-yo [2014/11/06 02:41] pwirving183_notes:examples:a_yo-yo [2014/11/06 02:59] (current) pwirving
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 ΔKtrans = fiFnetdrcm ΔKtrans = fiFnetdrcm
 +
 +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 it only has Ktrans)
 + 
 +ΔKtrans = fiFnetdrcm 
 + 
 +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 drcm we get:
  
 ΔKtrans=(Fmg)ΔyCM ΔKtrans=(Fmg)ΔyCM
  
-ΔyCM=h(fromdigram)+As indicated in diagram in the b section of the representation:
  
-ΔKtrans=(Fmg)(h)=(mgF)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} = (mg - F)h$
  
  
 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=(mgF)h (From part (a))+From part (a) of the problem we can substitute in (mgF)h for ΔKtrans as the translational kinetic energy will be the same. 
 + 
 +ΔKtrans=(mgF)h  
 + 
 +Substituting this into our equation leaves us with:
  
 (mgF)h+ΔKrot=Fd+mgh (mgF)h+ΔKrot=Fd+mgh
 +
 +Solve for change in rotational kinetic energy:
  
 ΔKrot=F(d+h) ΔKrot=F(d+h)
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