Proving the period of a pendulum

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    Pendulum Period
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Homework Help Overview

The discussion revolves around proving the periodicity of a pendulum's motion, specifically focusing on the period of the pendulum and the underlying differential equation governing its motion. Participants are exploring the relationship between the angular displacement and time, as well as the implications of initial conditions on the periodic behavior.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the need to clarify notation and initial conditions related to the differential equation of motion. There are attempts to establish the relationship between the values of angular displacement at different times and to explore the implications of symmetry in the motion.

Discussion Status

Some participants have offered clarifications regarding notation and have pointed out potential typos in the equations. There is an ongoing exploration of the implications of the periodic nature of the pendulum's motion, with various interpretations being considered. The discussion remains open with no explicit consensus reached.

Contextual Notes

There is a mention of the need for clearer definitions of initial conditions and the potential confusion arising from notation. Participants are also considering the implications of symmetry and time reversal in the context of the pendulum's motion.

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Homework Statement


I'm writing a small project as part of my degree, and I am stuck on proving one (probably simple!) thing towards the end. I've shown that the pendulum is periodic and has a total period of 4t2.

Homework Equations


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The Attempt at a Solution



I think I need to rewrite the same ODE with starting point t=0 but I'm having a complete mindblank on how to proceed from here. Any help would be greatly appreciated!
 
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Not entirely sure about your notation, nor what your starting points are.
You seem to be drawing on some earlier equation ##\ddot\theta=csin(\theta)##, but what is csin there? Do you just mean a constant c multiplied by sine? "csin" is a standard abbreviation for complex sine in some computer languages.
You also seem to know that ##\theta(t_2)=\dot\theta(t_2)=\dot\theta(0)=0##.
Anything else?
 
haruspex said:
n
Hi,

Sorry I should've given more information. The equation I'm drawing on as is as you said is ##\ddot\theta = -csin\theta## and this is just the regular sine function multiplied by a constant, c. No complex sine - sorry for the confusion.[PLAIN][PLAIN]http://blob:http://imgur.com/d719fbec-3e87-4f2c-a28f-955630eb054a [PLAIN][PLAIN]http://blob:http://imgur.com/d719fbec-3e87-4f2c-a28f-955630eb054a [PLAIN][PLAIN]http://blob:http://imgur.com/d719fbec-3e87-4f2c-a28f-955630eb054a [PLAIN][PLAIN]http://blob:http://imgur.com/d719fbec-3e87-4f2c-a28f-955630eb054a
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Here is everything I know that's relevant to periodicity in my paper. Thanks for your reply!
 
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The latex is clearer if you use \sin rather than just sin.

As far as I can see, nowhere did you define the initial conditions (t=0). But in the second stage (post #1) you use ##\dot\theta(0)=0##.

You have an equation ##\theta(t)=-\theta(4t_2-t)##.
What would that imply at t=2t2? Is the minus sign a mistake?
 
haruspex said:
The latex is clearer if you use \sin rather than just sin.

As far as I can see, nowhere did you define the initial conditions (t=0). But in the second stage (post #1) you use ##\dot\theta(0)=0##.

You have an equation ##\theta(t)=-\theta(4t_2-t)##.
What would that imply at t=2t2? Is the minus sign a mistake?
Noted for the future.

The minus sign is a typo, thanks for pointing that out!

At time t=2t2, we have that it's equal to ##\theta(-t)## by symmetry, since it's the furthest "left" position of the mass (taking moving from left to right as being negative).
 
I think I need to prove that ##\theta(4t_2) = \theta(0)## but I'm not entirely sure... I think to do that I would need to basically run through a very similar argument again and then use cauchy-lipschitz to show uniqueness
 
GetSchwifty said:
I think I need to prove that ##\theta(4t_2) = \theta(0)## but I'm not entirely sure... I think to do that I would need to basically run through a very similar argument again and then use cauchy-lipschitz to show uniqueness
You need to show that the initial conditions going forward from 4t2 are the same as those going forward from t=0. So that's the values of ##\theta## and ##\dot\theta##.
 
Thanks. It's very late here in the UK so I'll actually write this up tomorrow - the flu really isn't helping my thought process!

So in short I need to show that ##\theta(0) = \theta(4t_2)## and that ##\dot\theta(0) = \dot\theta(4t_2)##? And then use a similar argument from before, from my second post with:

$$\begin{cases}

\ddot y& = -csiny(t)\\

y(t_2)&=-\theta(2t_2-t_2)=-\theta(t_2)=0 \\

\dot y(t_2)&=\dot\theta(2t_2-t_2)=\dot\theta(t_2)

\end{cases}$$

Or am I way off?

And then I would need to change this to reflect 0 and ##4t_2##?

$$-\theta(2t_2-t)=\theta(t), t\in[t_2, 2t_2]$$
 
GetSchwifty said:
I need to show that ##\theta(0) = \theta(4t_2)## and that ##\dot\theta(0) = \dot\theta(4t_2)##?
Yes.
GetSchwifty said:
then use a similar argument
As you wish, but to me it would be suffice to say that the values of ##\theta## and ##\dot\theta## define the state of the system, so if the value pair recurs then the behaviour is cyclic. Likewise, for your antisymmetric result in post #3, I would just observe the effect of time reversal on the differential equation.
These are mechanistic arguments rather than purely mathematical ones.
 
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