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fisica1-youn-e-freedman-exercicios-resolvidos

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6.100: Use the Work–Energy Theorem, W = ∆KE,<br />

and integrate to find the work.<br />

x<br />

1 2<br />

∆KE<br />

= 0 − mv0 andW<br />

= ∫(<br />

−mg sin α − µ mg cos α)<br />

dx.<br />

2<br />

0<br />

Then,<br />

W<br />

= −mg<br />

x<br />

∫<br />

0<br />

(sin α + Ax<br />

cos α)<br />

dx,<br />

W<br />

⎡ Ax<br />

= −mg⎢sin<br />

αx<br />

+<br />

⎣ 2<br />

2<br />

⎤<br />

cos α ⎥.<br />

⎦<br />

Set W = ∆KE.<br />

2<br />

1 2 ⎡ Ax<br />

⎤<br />

− mv<br />

0<br />

= −mg<br />

sin cos .<br />

2<br />

⎢ αx<br />

+ α<br />

2<br />

⎥<br />

⎣<br />

⎦<br />

To eliminate x, note that the box comes to a rest when the force of static friction balances<br />

the component of the weight directed down the plane. So, mg sin α = Ax mg cos α;<br />

solve<br />

this for x and substitute into the previous equation.<br />

sin α<br />

x = .<br />

A cos α<br />

Then,<br />

1<br />

v<br />

2<br />

2<br />

0<br />

2<br />

⎡<br />

⎛ sin α ⎞ ⎤<br />

⎢<br />

A⎜<br />

⎟ ⎥<br />

⎢ sin α A cos<br />

sin<br />

⎝ α<br />

= + g<br />

cos<br />

⎥<br />

⎢<br />

α +<br />

⎠<br />

α ,<br />

A cos α 2 ⎥<br />

⎢<br />

⎥<br />

⎢⎣<br />

⎥⎦<br />

2<br />

2 3g<br />

sin α<br />

and upon canceling factors and collecting terms, v<br />

0<br />

= . Or the box will remain<br />

A cos α<br />

2<br />

2 3g<br />

sin α<br />

stationary whenever v0<br />

≥ .<br />

A cos α

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