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X(t) = a e^(-bt/2m) cos(ω't + φ)

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Intro to Mechanics

Definition

This equation represents the displacement of a damped harmonic oscillator over time. It captures how the amplitude of oscillation decreases exponentially due to damping while the system continues to oscillate at a modified frequency. The terms in the equation include an exponential decay factor and a cosine function, which illustrates the combined effects of damping and oscillatory motion.

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5 Must Know Facts For Your Next Test

  1. The term 'a' represents the initial amplitude of the oscillation before any damping occurs.
  2. The factor 'b' indicates the damping coefficient, which quantifies how quickly the oscillations lose energy over time.
  3. The term 'm' denotes mass, which plays a role in determining how quickly the oscillator responds to damping forces.
  4. The modified frequency 'ω'' is related to the natural frequency and decreases due to damping effects.
  5. As time progresses, the displacement x(t) approaches zero, demonstrating how energy is dissipated in damped oscillations.

Review Questions

  • How does the damping coefficient 'b' affect the behavior of the oscillator represented by x(t) = a e^(-bt/2m) cos(ω't + φ)?
    • The damping coefficient 'b' directly influences how quickly the amplitude of the oscillator decreases over time. A larger value of 'b' results in faster energy dissipation, leading to quicker reduction in oscillation amplitude. Conversely, a smaller value means that the system will retain its oscillatory motion for a longer duration before coming to rest, demonstrating slower energy loss.
  • Compare and contrast damped oscillations with undamped oscillations in terms of their mathematical representation and physical implications.
    • Damped oscillations, represented by x(t) = a e^(-bt/2m) cos(ω't + φ), exhibit an exponential decay in amplitude due to energy loss from damping forces. In contrast, undamped oscillations maintain a constant amplitude and are described by a simpler equation without the exponential decay term. Physically, damped systems eventually come to rest due to energy loss, while undamped systems continue to oscillate indefinitely without external influences.
  • Evaluate how varying initial conditions such as amplitude 'a' and phase angle 'φ' can affect the overall motion of a damped harmonic oscillator over time.
    • Varying initial conditions significantly influence the behavior of a damped harmonic oscillator. The initial amplitude 'a' determines how far the system initially displaces from its equilibrium position; larger amplitudes lead to larger maximum displacements throughout its motion. The phase angle 'φ' affects where in its cycle the motion begins, altering the timing of peaks and troughs in displacement. Together, these factors create diverse motion profiles even under identical damping conditions, showcasing the complexity of damped oscillations.

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