Starting from rest, a basketball rolls from the top to the bottom of a hill, reaching a translational speed of 6.5 m/s. Ignore frictional losses. (a) What is the height of the hill? (b) Released from rest at the same height, a can of frozen juice rolls to the bottom of the same hill. What is the translational speed of the frozen juice can when it reaches the bottom?
(a) Use the law of conservation of mechanical energy
incorporating both translational and rotational kinetic energy. The
moment of inertia, I, for the basketball is close to 2mr²/3:
mgh = mv²/2 + I?²/2
mgh = mv²/2 + (2mr²/3)(v/r)²/2
gh = 5v²/6
h = 5v²/6g
= 5(6.5m/s)²/6(9.8m/s²)
= 3.6m
(b) The value of I for a frozen orange juice can (which, I suppose,
would be modeled as a solid cylinder) would be close to mr²/2, so
it’s speed would be found similarly to part (a):
mgh = mv²/2 + (1/2)(mr²/2)(v/r)²
v = ?[4gh/3]
= ?[4(9.8m/s²)(3.6m)/3]
= 6.86m/s
Hope this helps.
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