p08_009.pdf

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Chapter 8 - 8.9
9. (a) If K i is the kinetic energy of the flake at the edge of the bowl, K f is its kinetic energy at the
bottom, U i is the gravitational potential energy of the flake-Earth system with the flake at the top,
and U f is the gravitational potential energy with it at the bottom, then K f + U f = K i + U i .Taking
the potential energy to be zero at the bottom of the bowl, then the potential energy at the top is
U i = mgr where r =0 . 220 m is the radius of the bowl and m is the mass of the flake. K i =0 since
the flake starts from rest. Since the problem asks for the speed at the bottom, we write 2 mv 2 for
K f . Energy conservation leads to
2 mv 2 =
v = 2 gr = 2(9 . 8)(0 . 220) =2 . 08 m / s .
(b) We note that the expression for the speed ( v = 2 gr ) does not contain the mass of the flake. The
speed would be the same, 2 . 08m / s, regardless of the mass of the flake.
(c) The final kinetic energy is given by K f = K i + U i
mgr = 1
U f .Since K i is greater than before, K f is
greater. This means the final speed of the flake is greater.
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