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fisica1-youn-e-freedman-exercicios-resolvidos

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2.66: a) The simplest way to do this is to go to a frame in which the freight train (which<br />

moves with constant velocity) is stationary. Then, the passenger train has<br />

an initial relative velocity of v rel,0 = 10 m s . This relative speed would be decreased to<br />

vrel<br />

,0<br />

zero after the relative separation had decreased to = + 500 m.<br />

Since this is larger in<br />

magnitude than the original relative separation of 200 m, there will be a collision. b) The<br />

time at which the relative separation goes to zero (i.e., the collision time) is found by<br />

solving a quadratic (see Problems 2.35 & 2.36 or Example 2.8). The time is given by<br />

2<br />

2arel<br />

2<br />

( vrel,0<br />

− vrel,0<br />

2axrel,0<br />

)<br />

1<br />

t =<br />

+<br />

a<br />

= (10 s<br />

2<br />

m)(10 m s −<br />

((1<br />

0.6)<br />

= ( 100 s) − .<br />

100 m<br />

2<br />

s<br />

2<br />

− 40 m<br />

Substitution of this time into Eq. (2.12), with x 0 = 0, yields 538 m as the distance the<br />

passenger train moves before the collision.<br />

2<br />

s<br />

2<br />

)<br />

2.67: The total distance you cover is 1 .20 m + 0.90 m = 2.10 m and the time available is<br />

1<br />

= 0.80 s . Solving Eq. (2.12) for a x ,<br />

.20 m<br />

1.50 m s<br />

( x − x ) − v<br />

t<br />

t<br />

(2.10 m) − (0.80m s)(0.80 s)<br />

(0.<br />

80 s)<br />

0 0x<br />

s<br />

2<br />

x<br />

= 2 = 2<br />

= 4.56 m .<br />

2<br />

2<br />

a

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