Motion of a non-linear pendulum with air resistance

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SUMMARY

The discussion focuses on modeling the motion of a non-linear pendulum with air resistance using the equations Fc = mgsin(theta) and Fdrag = (1/2)p(v^2)CA. The user initially struggles with obtaining a damped oscillating curve due to the term v^2 not changing signs. After suggestions to replace v^2 with |v|v and correcting sign errors in the force equations, the user successfully adjusts their model, leading to improved graph outputs. The final equation derived is θ'' = -g/L sin(θ) - (pLcA/2m) θ' |θ'|, with initial conditions θ(0) = 1.5 and θ'(0) = 0.

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Omkar Vaidya
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Homework Statement


I need to come up with an equation that would model the motion of a non-linear pendulum with air resistance. [/B]

Homework Equations


Fc=mgsintheta
Fdrag=(1/2)p(v^2)CA

The Attempt at a Solution



I started with mgsintheta-(1/2)p(v^2)CA=ma

After substituting v=r*omega and a=r*alpha, I get the following (look at the image)
i6bfv0


However, after graphing, I do not get a damped oscillating curve, because of the v^2 not changing signs. Can someone guide me? See second image:
i6bh0j
http://prntscr.com/i6bh0j[/B]

https://prnt.sc/i6bfv0
 
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Sorry, we can't see the 1st image
 
To know whether there is a problem, how many cycles did you follow it through?
 
epenguin said:
To know whether there is a problem, how many cycles did you follow it through?
I'm not quite sure what you mean by cycles. I set the domain on the graph to be [0, 2pi].
 
Omkar Vaidya said:
I'm not quite sure what you mean by cycles. I set the domain on the graph to be [0, 2pi].
To be sure there is no damping try 20π or 100π?
 
It does make sense that your damping doesn't work if the damping force is always pointing in the same direction and not against v. Maybe you should try to replace v^2 by |v|v.
 
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epenguin said:
To be sure there is no damping try 20π or 100π?
I did, and there does not seem to be any. However, the amplitude does seem to change, but on average it remains the same.
 
Gigaz said:
It does make sense that your damping doesn't work if the damping force is always pointing in the same direction and not against v. Maybe you should try to replace v^2 by |v|v.
Thanks, this does work. For some reason I didn't think of the absolute value as a solution to the v^2 problem. Now I get a graph that looks like the following. It does not pass through the x-axis like it should.
https://prnt.sc/i6cgpx
 
  • #10
Omkar Vaidya said:
Thanks, this does work. For some reason I didn't think of the absolute value as a solution to the v^2 problem. Now I get a graph that looks like the following. It does not pass through the x-axis like it should.
https://prnt.sc/i6cgpx

Another sign error. When you're at positive theta, the force must point in the negative direction. So it should be -mgsin(theta).
 
  • #11
Gigaz said:
Another sign error. When you're at positive theta, the force must point in the negative direction. So it should be -mgsin(theta).
yes, I thought I already changed that. Thanks again.
 
  • #12
Gigaz said:
Another sign error. When you're at positive theta, the force must point in the negative direction. So it should be -mgsin(theta).
Did you look at the derivation of that equation I came up with? I just need someone to check if its correct (apart from the signs, and absolute values)
 
  • #13
Omkar Vaidya said:
Did you look at the derivation of that equation I came up with? I just need someone to check if its correct (apart from the signs, and absolute values)

Seems fine to me.
 
  • #14
Gigaz said:
Seems fine to me.

Here is what I get using Maple to solve the IVP
$$\theta^{''} = -\frac{g}{L} \sin(\theta) - \frac{pLcA}{2m} \theta' |\theta'|, \; \theta(0)=1.5, \theta'(0)=0$$
using your input parameters (but using notation ##w(t)## instead of ##\theta(t)##):
upload_2018-1-27_9-12-58.png
 

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  • #15
Thread moved. Problems involving differential equations belong in the Calculus & Beyond section.
 

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