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Physics 101:  Lecture 9 Work and Kinetic Energy ,[object Object],Exam II
Energy ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],12
Energy is Conserved ,[object Object],[object Object],[object Object],[object Object],[object Object],10
Work: Energy Transfer due to Force ,[object Object],[object Object],[object Object],[object Object],[object Object],15 W = F dcos(  ) T a mg T b mg T b
Work by Constant Force ,[object Object],[object Object],W F  < 0:  90<    < 180 : cos(  ) < 0 W F  = 0:    =90 : cos(  ) =0 W F  < 0:  90<    < 180 : cos(  ) < 0 W F  > 0:  0<    < 90 : cos(  ) > 0 18 A) W>0 B) W=0 C) W<0 1) 2) 3) 4) Note Change in r! F   r F  r F  r F  r F  r F   r F 
ACTS: Ball Toss ,[object Object],[object Object],[object Object],[object Object],[object Object],20
Work by Constant Force ,[object Object],30 50 N W = F   x cos      m ) cos (30) = 217  Joules   21 T mg N f
Where did the energy go? ,[object Object],[object Object],[object Object],W = F   r cos    30 x 5 cos(90)  X-Direction:   F = ma T cos(30) – f = 0 f = T cos(30) W = F   r cos    50 cos(30)   x 5 cos(180)  Joules 25 mg 90  r T mg N f f  r 180
Preflight 1  ,[object Object],[object Object],T V “ Normal force is perpendicular to the direction of the car, so it does not contribute” 28 W F N correct
Preflight 2  ,[object Object],[object Object],“ The gravitational force is acting against the car going up the hill which makes it negative” 30 W T F N V correct
Preflight 3  ,[object Object],[object Object],“ The work done by the tow rope would be positive because the distance and force applied by the tow rope are both in the positive direction”  32 W T F N V correct
Kinetic Energy: Motion ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],35
Preflight 4  ,[object Object],[object Object],The net acceleration is 0 which means the sum of the forces is 0. Thus, work done is 0..  37 W T F N V correct
Example: Block w/ friction ,[object Object],5 m/s Y direction:   F=ma N-mg = 0 N = mg Work W N  = 0 W mg  = 0 W f  = f   x cos(180) = -  mg   x W =    K -  mg   x = ½ m (v f 2  – v 0 2 ) -  g   x = ½  (0 – v 0 2 )  g   x = ½ v 0 2  x = ½ v 0 2  /   g = 3.1 meters 44 mg N f x y
Falling Ball Example ,[object Object],Only force/work done by gravity  W =   KE W g  = ½  m (v f 2  – v i 2 ) F g  h cos(0) = ½m v f 2 mgh = ½m v f 2 V f  = sqrt( 2 g h ) = 10 m/s mg 47
Work by Variable Force ,[object Object],[object Object],[object Object],[object Object],Force Distance Work Work 49 Force Distance F=kx
Summary ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],50

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Lecture09

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Editor's Notes

  1. 1
  2. Maybe do example of conservation (like cookies) and counter example like acceleration
  3. Get demo
  4. W = f d cos(theta)
  5. On transparency