Dynamics_Part10

5

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Unformatted text preview: .............. ................................................... ...................................................... .... ... ... . . .. .. ... ... ..... ................................................. . . ... .... .. .. .. ... . ................................................ ............................................. ............................................ .......................................... . . . . . . ... .... ........................................ ................................... ..................................... .... . .. .. ... ... . ............................. ................................ .............................. ........................... ......................... . .. ... ..... ....................... ... .... ................... .................... 2 ................ .............. ............ .......... ........ .. .. . ..... v=V i x g = -g k So ut on: Because we gnore fr c on he mo on of he sk umper s sub ec on y o he cons an grav aona acce era on Deno ng me by t and e ng t = 0 when he sk umper aunches from he op of he s ope he equa ons and n a cond ons govern ng he mo on are d x =0 dt2 x(0) = 0 and x(0) = V d2 z = -g z(0) = 0 and z(0) = 0 dt2 (a) In egra ng w ce and mpos ng he n a cond ons he so u on o he equa ons for x and z s x(t) = V t When he sk umper ands a and 1 z(t) = - gt2 2 me we know ha x( ) = cos and z( ) = - s n = cos V 2 Therefore we have V = cos and 1 1 - s n = - g 2 = - g 2 2 cos V =...
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This note was uploaded on 05/12/2010 for the course AME 301 taught by Professor Shiflett during the Spring '06 term at USC.

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