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fisica1-youn-e-freedman-exercicios-resolvidos

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7.76: The kinetic energy K′ after moving up the ramp the distance s will be the energy<br />

initially stored in the spring, plus the (negative) work done by gravity and friction, or<br />

1 2<br />

K′<br />

= kx − mg(sinα + µ<br />

k<br />

cosα)<br />

s.<br />

2<br />

Minimizing the speed is equivalent to minimizing K′ , and differentiating the above<br />

d K′<br />

expression with respect to α and setting = 0 gives<br />

dα<br />

0 = −mgs<br />

(cosα − µ<br />

k<br />

sinα),<br />

1<br />

or tan α = , ⎛ 1<br />

µ<br />

⎟ ⎞<br />

α = arctan<br />

k<br />

⎜ . Pushing the box straight up ( α = 90°<br />

) maximizes the<br />

⎝ µ<br />

k ⎠<br />

vertical displacement h, but not s = h sinα<br />

.<br />

7.77: Let x = 0.18<br />

1<br />

m , x = 0.71 m<br />

2<br />

. The spring constants (assumed identical) are then<br />

known in terms of the unknown weight w, 4 kx<br />

1<br />

= w . The speed of the brother at a given<br />

height h above the point of maximum compression is then found from<br />

1 2 1 ⎛ w ⎞<br />

(4k)<br />

x<br />

2<br />

2<br />

= ⎜ ⎟ v + mgh,<br />

2 2 ⎝ g ⎠<br />

or<br />

v<br />

2<br />

2<br />

(4k)<br />

g 2<br />

⎛ x ⎞<br />

2<br />

= x2<br />

− 2gh<br />

= g<br />

⎜ − 2h<br />

⎟,<br />

w<br />

⎝ x1<br />

⎠<br />

2<br />

2<br />

so v = (9.80 m s ) ((0.71 m) (0.18 m) − 2(0.90 m)) = 3.13 m s , or 3 .1 m s to two<br />

figures. b) Setting v = 0 and solving for h,<br />

2 2<br />

2kx2 x2<br />

h = = = 1.40 m,<br />

mg 2x<br />

or 1.4 m to two figures. c) No; the distance x<br />

1<br />

will be different, and the ratio<br />

0.53 m<br />

( ) 2<br />

2<br />

2<br />

x2 ( x1<br />

0.53 m)<br />

x1<br />

x<br />

= x<br />

1<br />

1<br />

1+<br />

x1<br />

= + will be different. Note that on a small planet, with lower g,<br />

x will be smaller and h will be larger.<br />

1<br />

1

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