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Physics 101:  Lecture 16  Angular Momentum ,[object Object],Exam II
Overview ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Linear and Angular ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Today
Define Angular Momentum Momentum Angular Momentum p = mV   L = I  conserved if   F ext  = 0 conserved if   ext  =0 Vector Vector! units:  kg-m/s units:  kg-m 2 /s
Right Hand Rule ,[object Object],[object Object],[object Object]
Act: Two Disks ,[object Object],[object Object], i Wheel rim drop z  f z
Act: Two Disks ,[object Object],[object Object], 0 z 2 1  f z
Lecture 16,   Pre-flights ,[object Object],[object Object]
Bonus Question! ,[object Object],[object Object],Key is no external torques about vertical axis! FBD has gravity and normal force.
Lecture 16,   Preflight 1  ,[object Object],[object Object],“ Because there are no external torques present, angular momentum is conserved ” L 1 L 2 CORRECT
Lecture 16,   Preflight 2 ,[object Object],[object Object],“ you decreased the I so w increases ”   “ I tried this out Friday night ” “ thanks for the new drinking game”  1    2   I 2   I 1   L L CORRECT
Lecture 16,   Preflight 3 ,[object Object],[object Object],“ KE is inversly related to intertia, therefore, increases.” CORRECT  1    2   I 2   I 1   L L (using  L = I    )
What about Energy Conservation? ,[object Object],[object Object],[object Object],[object Object],[object Object]
Turning the bike wheel ,[object Object],[object Object],Start w/ angular momentum L pointing up from wheel. When wheel is flipped, no more angular momentum from it pointing up, so need to spin person/stool to conserve L! CORRECT
Turning the bike wheel (more) ,[object Object],[object Object]
Turning the bike wheel... ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],L W,F  L S  L W,I  L W,I  =  L W,F   +   L S
Act 2  Rotations  ,[object Object],(a)   2  (b)   4  (c)  8   Puck on ice
Act 2  Solution ,[object Object],L 1  =  I 1  1  = mR 2  1    m R    m R/2 L 2  =  I 2  2  = m   2 = mR 2  1  = m  R 2  2  1  =    2  2  = 4  1
Gyroscopic Motion: ,[object Object],[object Object], pivot support g
Gyroscopic Motion... ,[object Object],[object Object],[object Object], pivot g
Gyroscopic Motion... ,[object Object], pivot Bicycle wheel
Summary ,[object Object],[object Object],[object Object],[object Object]

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Lecture16

  • 1.
  • 2.
  • 3.
  • 4. Define Angular Momentum Momentum Angular Momentum p = mV L = I  conserved if  F ext = 0 conserved if  ext =0 Vector Vector! units: kg-m/s units: kg-m 2 /s
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  • 6.
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Editor's Notes

  1. 1
  2. Note in example w/ hubs, energy was lost.