What Role Do Weight and Friction Play in SHM with F = -kx?

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Discussion Overview

The discussion centers on the role of weight and friction in simple harmonic motion (SHM) described by the equation F = -kx. Participants explore the implications of additional forces, such as air resistance and friction, on the idealized model of SHM, particularly in the context of a mass on a linear air track.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions whether the force F = -kx only refers to the restoring force from the springs, or if it also accounts for air resistance acting on the gliding object.
  • Another participant acknowledges that friction is horizontal but suggests it is negligible, indicating that the motion will closely resemble SHM.
  • A participant seeks clarification on whether the 'unclosed-system' quality should be explained by the weight's contribution to friction rather than its vector direction relative to the spring force.
  • One participant proposes a distinction between the restoring force from springs and the air resistance, suggesting that increased mass leads to increased damping due to additional friction beyond just air resistance.

Areas of Agreement / Disagreement

Participants express uncertainty regarding the interactions between weight, friction, and the forces described by F = -kx. There is no consensus on how to best characterize the effects of these additional forces on the system.

Contextual Notes

Participants note the limitations of the SHM model in accounting for real-world factors such as air resistance and friction, indicating that the system is not closed. The discussion highlights the complexity of these interactions without resolving the implications.

Who May Find This Useful

This discussion may be of interest to students and educators in physics, particularly those exploring the nuances of simple harmonic motion and the effects of external forces on idealized models.

linyen416
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SHM --> F = -kx

SHM assumes that F is the only force acting on the system, so if we have a mass held between two springs on a linear air track, the F = -kx
force refers to the restoring force from the springs?

Is that the only thing it refers to? What about air resistance as the gliding object travels horizontally along the air track?



I've noticed also that the weight of the gliding object introduces friction so it's not exactly a closed system, could I explain this by saying that this is because F = -kx which acts horizontally, is perpendicular to the force of the weight? So F = -kx does not accoutn for the friction introduced by weight?

Or am I wrong to say that becase the friction introduced by the weight is acting horizontally as well?

I'm confounded.
 
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linyen416 said:
Or am I wrong to say that becase the friction introduced by the weight is acting horizontally as well?

Hi linyen416! :smile:

Yes, the friction is horizontal.

But it's very small, so the motion will be very very nearly SHM (just like an ordinary pendulum, for example). :smile:
 


so I shouldn't explain the 'unlcosed-system' quality by saying that the wt force acts in a different vector componenet as the force from springs, but rather I should explain it by saying that the friction is introduced by the weight pushing down, so it's not exactly closed?
 


so to clear things up:
F = -kx refers to restorative force from springs
F = -bv refers to the air resistance as the glider moves along

and so if we use our amplitude -time graphs to calculated b, we should find that as m increases, b increases because the non-closed system causes extra friction to be introduced, therefore extra damping other than just air restistance.
 

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