Chapter 11
Its final kinetic energy (as it leaves the roof) is (Eq. 11-5) . Here we use v to denote the speed of its center of mass and is its angular speed — at the moment it leaves the roof. Since (up to that moment) the ball rolls without sliding we can set v = R = v where R = 0.10 m. Using (Table 10-2(c)), conservation of energy leads to . The mass M cancels from the equation, and we obtain (b) Now ... ................
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