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2 249 m s<br />

2.47: a) (224 m s) (0.9 s) = 249 m s . b) = 25.4.<br />

c) The most direct way to<br />

2<br />

9.80 m s<br />

ave<br />

t = ((224 m s) 2)(0.9 s) =<br />

find the distance is v<br />

101m.<br />

2<br />

d) ( 283 m s) (1.40 s) = 202 m s but 40 g = 392 m s , so the figures are not consistent.<br />

2<br />

2<br />

2.48: a) From Eq. (2.8), solving for t gives (40.0 m s – 20.0 m s )/9.80<br />

b) Again from Eq. (2.8),<br />

40.0 m s − ( −20.0<br />

m s)<br />

9.80 m s<br />

2<br />

=<br />

6.12 s.<br />

2<br />

m s = 2.04 s.<br />

c) The displacement will be zero when the ball has returned to its original vertical<br />

position, with velocity opposite to the original velocity. From Eq. (2.8),<br />

40 m s − ( −40<br />

m s)<br />

9.80 m s<br />

(This ignores the t = 0 solution.)<br />

d) Again from Eq. (2.8), (40 m s )/(9.80<br />

time found in part (c).<br />

2<br />

e) 9.80 m s , down, in all cases.<br />

f)<br />

2<br />

=<br />

8.16 s.<br />

2<br />

m s ) = 4.08 s. This is, of course, half the

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