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5.96: (a) 80 mi h is 35 .7 m s in SI units. The centripetal force needed to keep the car on<br />

the road is provided by friction; thus<br />

2<br />

mv<br />

µ mg =<br />

s<br />

r =<br />

r<br />

2<br />

2<br />

v (35.7 m s)<br />

=<br />

= 171m or 170 m<br />

2<br />

µ g (0.76)(9.8 m s )<br />

s<br />

(b) If µ = 0.20<br />

s<br />

:<br />

2<br />

2<br />

2<br />

v = rµ<br />

sg<br />

= (171m) (0.20) (9.8 m s ) = 335.2 m<br />

v = 18.3 m s or about 41mi h<br />

(c) If µ = 0.37<br />

s<br />

:<br />

2<br />

2<br />

2<br />

v = (171m) (0.37) (9.8 m s ) = 620 m<br />

2<br />

s<br />

v = 24.9 m s or about 56 mi h<br />

The speed limit is evidently designed for these conditions.<br />

s<br />

2<br />

5.97: a) The static friction force between the tires and the road must provide the<br />

centripetal acceleration for motion in the circle.<br />

2<br />

v<br />

µ mg s<br />

= m<br />

r<br />

v1<br />

v2<br />

m, g, and r are constant so = , where 1 refers to dry road and 2 to wet<br />

µ µ<br />

road.<br />

1<br />

µ , s 2<br />

=<br />

2<br />

µ<br />

s1<br />

so v2<br />

= (27 m s) 2 = 19 m s<br />

b) Calculate the time it takes you to reach the curve<br />

v = 27 m s, v = 19 m s, x − x = 800 m, t = ?<br />

0x<br />

x<br />

s1<br />

0<br />

s2<br />

⎛ v0x<br />

+ vx<br />

⎞<br />

x − x0<br />

= ⎜ ⎟ t gives t = 34.7 s<br />

⎝ 2 ⎠<br />

During this time the other car will travel x − x0 = v0<br />

x<br />

t = (36 m s) (34.7s) = 1250 m. The<br />

other car will be 50 m behind you as you enter the curve, and will be traveling at nearly<br />

twice your speed, so it is likely it will skid into you.<br />

5.98: The analysis of this problem is the same as that of Example 5.22; solving for v in<br />

2<br />

terms of β and R , v = gR tan β = (9.80 m s ) (50.0) tan 30.0°<br />

= 16.8 m s, about<br />

60 .6 km<br />

h.

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