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2.20: a) The bumper’s velocity and acceleration are given as functions of time by<br />

dx<br />

2<br />

6 5<br />

v x<br />

= = ( 9.60 m s ) t − (0.600 m s ) t<br />

dt<br />

dv<br />

2<br />

6 4<br />

a x<br />

= = (9.60 m s ) − (3.000 m s ) t .<br />

dt<br />

There are two times at which v = 0 (three if negative times are considered), given by t =<br />

0 and t 4 = 16 s 4 . At t = 0, x = 2.17 m and a x = 9.60 m s<br />

2 . When t 4 = 16 s 4 ,<br />

b)<br />

x = (2.17 m) + (4.80 m s<br />

2 ) (16 s<br />

4 ) – (0.100)<br />

a x = (9.60<br />

m s<br />

2 ) – (3.000<br />

6<br />

m s )(16 s 4 ) 3/2 = 14.97 m,<br />

6<br />

m s )(16 s 4 ) = –38.4 m s<br />

2 .<br />

2.21: a) Equating Equations (2.9) and (2.10) and solving for v 0 ,<br />

2(<br />

x − x0<br />

) 2(70 m)<br />

v0 x<br />

= − vx<br />

= −15.0 m s = 5.00 m s.<br />

t 7.<br />

00 s<br />

b) The above result for v 0x may be used to find<br />

vx<br />

− v 15.0 m s 5.00 m s<br />

0 x<br />

−<br />

2<br />

a = =<br />

1.43 m s ,<br />

t<br />

7.00 s<br />

=<br />

x<br />

or the intermediate calculation can be avoided by combining Eqs. (2.8) and (2.12) to<br />

eliminate v 0x and solving for a x ,<br />

⎛ vx<br />

x − x0 ⎞ ⎛15.0<br />

m s 70.0 m ⎞<br />

2<br />

ax<br />

= 2⎜<br />

− 2<br />

= 1.43 m s .<br />

2<br />

⎟ =<br />

⎜ −<br />

2<br />

7.00 s (7 00 s)<br />

⎟<br />

⎝ t t ⎠ ⎝<br />

. ⎠

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