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10.1: Equation (10.2) or Eq. (10.3) is used for all parts.<br />

a) ( 4.00 m)(10.0 N) sin 90° = 40.00 N ⋅ m, out of the page.<br />

b) ( 4.00 m)(10.0 N) sin 120° = 34.6 N ⋅ m, out of the page.<br />

c) ( 4.00 m)(10.0 N) sin 30° = 20.0 N ⋅ m, out of the page.<br />

d) ( 2.00 m)(10.00 N) sin 60° = 17.3 N ⋅ m, into the page.<br />

e) The force is applied at the origin, so τ = 0.<br />

f) ( 4.00 m)(10.0 N) sin 180°<br />

= 0.<br />

10.2: τ<br />

1<br />

= −(8.00 N)(5.00 m) = −40.0 N ⋅ m,<br />

τ = (12.0 N)(2.00 m) sin 30°<br />

= 12.0 N<br />

2<br />

⋅<br />

where positive torques are taken counterclockwise, so the net torque is − 28.0 N ⋅ m, with<br />

the minus sign indicating a clockwise torque, or a torque into the page.<br />

m,<br />

10.3: Taking positive torques to be counterclockwise (out of the page),<br />

τ = − 0.090 m) × (180.0 N) = −1.62 N ⋅ m, τ = (0.09 m)(26.0 N) = 2.34 N<br />

1<br />

(<br />

2<br />

⋅<br />

3<br />

= ( 2)<br />

(0.090 m) (14.0 N) = 1.78 N ⋅ m,<br />

.50 N<br />

τ so the net torque is 2 ⋅ m, with the<br />

direction counterclockwise (out of the page). Note that for τ<br />

3<br />

the applied force is<br />

perpendicular to the lever arm.<br />

m,<br />

10.4: τ<br />

1<br />

+ τ2<br />

= −F1<br />

R + F2<br />

R = ( F2<br />

− F1<br />

) R<br />

= ( 5.30 N − 7.50 N)(0.330 m) = −0.726 N ⋅ m.<br />

10.5: a)<br />

b) Into the plane of the page.<br />

r<br />

c) F<br />

r<br />

× = [( −0.450 m) iˆ<br />

+ (0.150 m) ˆ] j × [( −5.00 n)ˆ i + (4.00 N)ˆ i ]<br />

= ( −0.450 m) (4.00 N) − (0.150 m)( −5.00 N) kˆ<br />

= ( −1.05 N ⋅ m) kˆ

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