Displacement in SHM: Arc or Line from Mean Position?

AI Thread Summary
In the discussion about displacement in simple harmonic motion (SHM) for an oscillating pendulum, participants debate whether displacement should be measured as the arc length of the pendulum's path or the straight-line distance from the mean position. It is clarified that while angular displacement θ is typically used, for small angles, straight-line displacement can be approximated as Lθ, which is derived from the arc length. However, this approximation holds true primarily for small angles, as larger angles lead to non-linear behavior, deviating from SHM. The conversation also touches on the importance of understanding the limitations of these approximations and the role of restoring forces in SHM. Ultimately, both arc length and straight-line distance can be used as coordinates, but their applicability depends on the angle of displacement.
andyrk
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For SHM of oscillating pendulum, when the pendulum is at the extreme position, what is considered as the displacement? The curve/arc of the circle the bob is following or the straight line distance from the mean position?
 
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It is the curve or arc of the circle the bob is following.
 
But shouldn't it be the straight line displacement from the mean position?
 
andyrk said:
For SHM of oscillating pendulum, when the pendulum is at the extreme position, what is considered as the displacement?

andyrk said:
But shouldn't it be the straight line displacement from the mean position?

Technically , for SHM of a pendulum we use angular diplacement θ rather than straight line displacement . However as θ is a small we can still use straight line displacement . This is approximately equal to the length of the arc .
 
What if θ is not small?
 
Then you wouldn't have SHM .
 
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andyrk said:
What if θ is not small?
What do your textbooks tell you about these questions you are asking on PF? Yet again, this topic is well covered on line and in books.
 
I don't know. They didn't mention if it was small or not. But they have taken the displacement to be ##lθ##. So I think that must mean that θ is small. Am I right?
 
Yes. As qwerty said, Lθ is just an approximation for Lsinθ, but this approximation is only accurate for small angles.
If you know about taylor series, you can look at the taylor series for sinθ and see where this approximation comes from (the smaller θ, the smaller the effect of the higher order terms).
If you don't know about taylor series then you can understand this approximation geometrically, too. But if that's the case then you should go study taylor series! Useful stuff..
 
  • #10
andyrk said:
I don't know. They didn't mention if it was small or not. But they have taken the displacement to be ##lθ##. So I think that must mean that θ is small. Am I right?
SHM is a specific kind of oscillation - the simplest there is, in fact. SHM requires the restoring force to be directly proportional to the displacement and, for a simple pendulum, it is not. Look at this link, which shows that the motion of a simple pendulum 'approaches' pure SHM as the amplitude approaches zero.
 
  • #11
Do you know the derivation for SHM ?
 
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Some old clockmakers went to considerable trouble to make the motion of their pendulums follow SHM as near as possible at practical angles of swing . They did this by devising ways of making the effective length of the pendulum change slightly as it swung back and forth .
 
  • #13
andyrk said:
For SHM of oscillating pendulum, when the pendulum is at the extreme position, what is considered as the displacement? The curve/arc of the circle the bob is following or the straight line distance from the mean position?
You can use either one as a coordinate. You can also use the angle, as it was already mentioned.
In general, for a system, there is more than one way to choose the coordinates. Some may be more convenient but not in anyway "correct" or "wrong".
But even if you use the straight distance, the motions is SHM only approximately, for small angles.

And the length of the arc is Lθ for any value of the angle. Is not an approximation.
The straight distance though, is only approximately so, for small angles.
 
  • #14
nasu said:
You can use either one as a coordinate. You can also use the angle, as it was already mentioned.
In general, for a system, there is more than one way to choose the coordinates. Some may be more convenient but not in anyway "correct" or "wrong".
But even if you use the straight distance, the motions is SHM only approximately, for small angles.

And the length of the arc is Lθ for any value of the angle. Is not an approximation.
The straight distance though, is only approximately so, for small angles.
Yes but, if you are using the arc in your equation, the restoring 'force' becomes a torque and that is not proportional to the angle in any case. It's still non linear with change of position.
 
  • #15
andyrk said:
I don't know. They didn't mention if it was small or not.
I don't know who the "they" you refer to were. If they were showing you the proper derivation of SHM, they would have included the limiting case for small angles.
 
  • #16
Did I say that it becomes linear if the angle is used?

The last part was a separate point. Someone said in a previous post that s=Lθ it is just an approximation for small theta, which is not true. I did not mean (and did not say)that the motion becomes SHM.
 
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  • #17
nasu said:
Did I say that it becomes linear if the angle is used?

The last part was a separate point. Someone said in a previous post that s=Lθ it is just an approximation for small theta, which is not true. I did not mean (and did not say)that the motion becomes SHM.
It bothered me that it may have been interpreted wrongly. You were discussing a change of co ordinates. The result is that the non linearity turns up somewhere else and that point needs to be made constantly, IMO.
 

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