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fisica1-youn-e-freedman-exercicios-resolvidos

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7.85: a) For the given proposed potential U ( x),<br />

−<br />

dU = −kx<br />

+ F , so this is a possible<br />

2<br />

potential function. For this potential, U (0) = − F 2k<br />

, not zero. Setting the zero of<br />

potential is equivalent to adding a constant to the potential; any additive constant will not<br />

change the derivative, and will correspond to the same force. b) At equilibrium, the force<br />

is zero; solving − kx + F = 0 for x gives x<br />

0<br />

= F k . U ( x ) 2<br />

0<br />

= − F k , and this is a<br />

minimum of U, and hence a stable point.<br />

c)<br />

dx<br />

d) No; F 0 at only one point, and this is a stable point. e) The extreme values of x<br />

tot<br />

=<br />

correspond to zero velocity, hence zero kinetic energy, so U ( x ) ±<br />

= E , where x<br />

±<br />

are the<br />

extreme points of the motion. Rather than solve a quadratic, note that<br />

1 2 2<br />

2<br />

k( x − F k)<br />

− F k , so U ( x ) ±<br />

= E becomes 2<br />

2<br />

1 ⎛ F ⎞ F<br />

k⎜<br />

x±<br />

− ⎟ − F k =<br />

2 ⎝ k ⎠ k<br />

F F<br />

x±<br />

− = ± 2 ,<br />

k k<br />

F F<br />

x+<br />

= 3 x−<br />

= − .<br />

k k<br />

f) The maximum kinetic energy occurs when U (x)<br />

is a minimum, the point x = F k<br />

found in part (b). At this point<br />

v = 2F mk .<br />

2<br />

2<br />

2<br />

K = E −U<br />

= ( F k)<br />

− ( − F k)<br />

= 2F<br />

k , so<br />

0

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