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11.46: a) Denote the weight per unit length<br />

as α , so w1 = α(10.0 cm), w2<br />

= α(8.0 cm), and w3<br />

= αl.<br />

The center of gravity is a distance xcm<br />

to the right of point O where<br />

x<br />

cm<br />

=<br />

w1<br />

(5.0 cm) + w2<br />

(9.5 cm) + w3<br />

(10.0 cm − l<br />

w + w + w<br />

1<br />

2<br />

3<br />

2)<br />

(10.0 cm)(5.0 cm) + (8.0 cm)(9.5 cm) + l(10.0 cm − l<br />

=<br />

(10.0 cm) + (8.0 cm) + l<br />

2)<br />

.<br />

Setting x 0 gives a quadratic in l , which has as its positive root cm.<br />

cm =<br />

l = 28.8<br />

b) Changing the material from steel to copper would have no effect on the length l<br />

since the weight of each piece would change by the same amount.<br />

r r v<br />

11.47: Let ′<br />

i<br />

=<br />

i<br />

− R ,where R r is the vector from the point O to the point P.<br />

r r r<br />

The torque for each force with respect to point P is then τ ′ =<br />

′× F , and so the net torque<br />

is<br />

∑<br />

r<br />

τ<br />

i<br />

=∑<br />

= ∑<br />

= ∑<br />

r<br />

r<br />

r<br />

( i<br />

− R) × Fi<br />

r r r r<br />

i<br />

× Fi<br />

− ∑ R × Fi<br />

r r r r<br />

i<br />

× Fi<br />

− R × ∑Fi.<br />

In the last expression, the first term is the sum of the torques about point O, and the<br />

second term is given to be zero, so the net torques are the same.<br />

i<br />

i<br />

i<br />

11.48: From the figure (and from common sense), the force F r 1<br />

is directed along the<br />

length of the nail, and so has a moment arm of (0.0800 m) sin 60°<br />

. The moment arm of<br />

F r 2<br />

is 0.300 m, so<br />

(0.0800 m) sin 60°<br />

F<br />

2<br />

= F1<br />

= (500 N)(0.231) = 116 N.<br />

(0.300 m)

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