Change in the amplitude of a damped spring block oscillator

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SUMMARY

The discussion centers on the analysis of a damped spring block oscillator, specifically examining how the amplitude decreases uniformly with each oscillation cycle. The equation derived, $$\Delta \mathbf{E} = E_f - E_i = \frac{1}{2}kx_0^2 - \frac{1}{2}k(x_0-\Delta x)^2 = f \cdot D$$, illustrates the energy loss due to friction, where $$\Delta x$$ represents the change in amplitude and D is the distance traveled in one oscillation. The challenge lies in accurately determining D, considering the diminishing distance to equilibrium after each oscillation. The weak friction force allows for the approximation of harmonic motion, emphasizing the relationship between energy loss and amplitude reduction.

PREREQUISITES
  • Understanding of harmonic motion principles
  • Familiarity with energy conservation in oscillatory systems
  • Knowledge of spring constants and their role in oscillation
  • Basic calculus for analyzing changes in amplitude
NEXT STEPS
  • Explore the derivation of the equation for energy loss in damped oscillators
  • Study the effects of varying spring constants on oscillation amplitude
  • Learn about the mathematical modeling of damped harmonic motion
  • Investigate numerical methods for simulating damped oscillations
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Students studying physics, particularly those focusing on mechanics and oscillatory motion, as well as educators seeking to enhance their understanding of damped systems in practical applications.

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Homework Statement


A block is acted on by a spring with spring constant k and a weak friction force of constant magnitude f . The block is pulled distance x0 from equilibrium and released. It oscillates many times and eventually comes to rest.

Show that the decrease of amplitude is the same for each cycle of oscillation.

2. The attempt at a solution
$$\Delta \mathbf{E} = E_f -E_i = \frac{1}{2}kx_0^2 - \frac{1}{2}k(x_0-\Delta x)^2 = f \cdot D$$
where ##\Delta x## is the change in amplitude after one oscillation and D is the distance traveled by the block in one oscillation. I am stuck here. How do I find D? It can't simply be 4x_0 because the distance from the point of rest to the equilibrium decreases on every half oscillation. Where do I go from here?
 
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The friction force is assumed weak, so you can approximate the leading order effect by assuming harmonic motion and ##\Delta x \ll x_0##.
 

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