banim max WWMF=0 im(-Va x = 0 x= X (a) (b) F = 0 Vmax K(-XP WWWm х%3 -х х- о (c) (d) x = 0 x= X (e) Figure 16.24 The transformation of energy in simple harmonic motion is illustrated for an object attached to a spring on a frictionless surface.

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Chapter1: Units, Trigonometry. And Vectors
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Damping oscillatory motion is important in many systems, and the ability to control the damping is even more so. This is generally attained using non-conservative forces such as the friction between surfaces, and viscosity for objects moving through fluids. The following example considers friction. Suppose a 0.200-kg object is connected to a spring as shown, but there is simple friction between the object and the surface, and the coefficient of friction μk is equal to 0.0800.                                                                          (a) What is the frictional force between the surfaces?                                      (b) What total distance does the object travel if it is released 0.100 m from equilibrium, starting at v = 0 ? The force constant of the spring is k = 50.0 N/m .

banim
max
WWMF=0 im(-Va
x = 0 x= X
(a)
(b)
F = 0 Vmax
K(-XP WWWm
х%3 -х х- о
(c)
(d)
x = 0 x= X
(e)
Figure 16.24 The transformation of energy in simple harmonic motion is illustrated for an object attached to a spring on a frictionless surface.
Transcribed Image Text:banim max WWMF=0 im(-Va x = 0 x= X (a) (b) F = 0 Vmax K(-XP WWWm х%3 -х х- о (c) (d) x = 0 x= X (e) Figure 16.24 The transformation of energy in simple harmonic motion is illustrated for an object attached to a spring on a frictionless surface.
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