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6.68: From Eq. (6.7), with x = 1<br />

0 ,<br />

x 2 x<br />

2 3 k 2 b 3 c 4<br />

W = ∫ Fdx =<br />

2 2 2<br />

0 ∫<br />

2<br />

( kx − bx + cx ) dx = x − x + x<br />

0<br />

2 3 4<br />

2<br />

2 3<br />

3 4<br />

= (50.0 N / m) x − (233 N / m ) x + (3000 N / m ) x<br />

2<br />

a) When x = 0.050<br />

2<br />

m , W = 0.115 J , or 0.12 J to two figures. b) When<br />

x2 = −0.050 m, W = 0.173 J , or 0.17 J to two figures. c) It’s easier to stretch the spring;<br />

2<br />

the quadratic − bx term is always in the − x -direction, and so the needed force, and<br />

hence the needed work, will be less when x > 2<br />

0 .<br />

2<br />

2<br />

(0.70 m/s)<br />

6.69: a) T ma = m v = 0.120kg) = 0.147 N , or 0.15 N to two figures. b) At<br />

=<br />

rad<br />

(<br />

R<br />

(0.<br />

40 m)<br />

(2.80 m/s)<br />

the later radius and speed, the tension is ( 0.120kg) = 9.41N<br />

(0. 10 m)<br />

, or 9.4 N to two<br />

figures. c) The surface is frictionless and horizontal, so the net work is the work done by<br />

the cord. For a massless and frictionless cord, this is the same as the work done by the<br />

person, and is equal to the change in the block’s kinetic energy,<br />

2 2<br />

2<br />

2<br />

K<br />

2<br />

− K1<br />

= (1/ 2) m(<br />

v2<br />

− v1<br />

) = (1/ 2)(0.120 kg)((2.80 m /s) − (0.70 m /s) ) = 0.441J . Note<br />

that in this case, the tension cannot be perpendicular to the block’s velocity at all times;<br />

the cord is in the radial direction, and for the radius to change, the block must have some<br />

non-zero component of velocity in the radial direction.<br />

6.70: a) This is similar to Problem 6.64, but here α > 0 (the force is repulsive), and<br />

x < , so the work done is again negative;<br />

2<br />

x 1<br />

⎛ 1 1 ⎞<br />

W = α<br />

⎜ −<br />

⎟ = (2.12×<br />

10<br />

⎝ x1<br />

x2<br />

⎠<br />

= −2.65×<br />

10<br />

Note that x<br />

1<br />

is so large compared to<br />

(6.13)) and solving for v<br />

2<br />

,<br />

2<br />

−26<br />

−17<br />

N ⋅ m<br />

J.<br />

2<br />

x that the term<br />

2<br />

2<br />

((0.200 m<br />

1<br />

−1<br />

2<br />

) − (1.25×<br />

10<br />

9<br />

m<br />

−1<br />

))<br />

1<br />

x<br />

is negligible. Then, using Eq.<br />

−17<br />

2 W<br />

5 2 2( −2.65×<br />

10 J)<br />

v<br />

2<br />

= v1<br />

+ = (3.00×<br />

10 m /s) +<br />

= 2.41×<br />

10<br />

−27<br />

m<br />

(1.67 × 10 kg)<br />

α<br />

b) With K2 = 0,<br />

W = −K1. Using W = − ,<br />

2 5<br />

x 2<br />

m/s.<br />

−26<br />

2<br />

α 2α<br />

2(2.12×<br />

10 N ⋅ m )<br />

−10<br />

x<br />

2<br />

= = =<br />

= 2.82×<br />

10 m.<br />

2<br />

−27<br />

5 2<br />

K1<br />

mv1<br />

(1.67 × 10 kg)(3.00×<br />

10 m/s)<br />

c) The repulsive force has done no net work, so the kinetic energy and hence the speed of<br />

5<br />

the proton have their original values, and the speed is 3.00× 10 m / s .

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