Why Does a Simple Pendulum Only Exhibit SHM at Small Angles?

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    Pendulum Shm
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Discussion Overview

The discussion centers on why a simple pendulum exhibits simple harmonic motion (SHM) only at small angles close to the equilibrium position. It explores the relationship between the angle of displacement and the nature of the restoring force, as well as implications for the period of the pendulum's motion.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested

Main Points Raised

  • Some participants suggest that the restoring force is not linear and is only approximately linear at small amplitudes, which is crucial for SHM.
  • Others propose that at extreme angles, such as 180 degrees, the period becomes infinite, indicating that the simple formula for the period is no longer valid as amplitude increases.
  • A participant explains that resolving the gravitational force into components shows that the parallel acceleration is proportional to sin(θ), which approximates θ for small angles, leading to SHM. For larger angles, this approximation fails, complicating the analysis.
  • Another participant notes that at larger angles, the pendulum exhibits slight vibrations, suggesting it is no longer undergoing SHM alone.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the nature of the restoring force and its implications for SHM, indicating that the discussion remains unresolved.

Contextual Notes

The discussion highlights the dependence on the angle of displacement and the limitations of the linear approximation for larger angles, but does not resolve the implications of these factors on the pendulum's motion.

sexysam_short
Why is it that a simple pendulum only shows SHM at small angles close to the equilibrium position?
 
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Because the restoring force is not linear and is only approximately linear at small amplitudes.
 
Consider that if the launch angle of the bob is 180 degrees (the "string" would have to rigid to maintain the length), the bob would balance there. Effectively this means the period is infinite for amplitude 180 degrees. It is easy to see then that as the amplitude becomes larger, the period is no longer given by the simple formula (i.e. constant independent of amplitude), but will increase.
 
If you resolve the gravitational force on a pendulum bob at angle θ to the vertical into a component perpendicular to the circular path (which just puts tension on the pendulum arm) and the component parallel to the path (which accelerates and decelerates the pendulum) you find that, from the right triangle set up, the parallel acceleration is proportional to sin(θ). For small values of θ that is very close to θ itself. It is that simplicity: acceleration= θ that gives "simple harmonic motion". For larger angles, we would have to use sin(&theta); instead of θ and that gives a much harder problem.
 
Also, something I've noticed is when the angle is fairly large, the pendulum begins to slightly vibrate as it swings. This indicates it's no longer undergoing SHM alone.
 
Last edited:

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