Deriving the Time Period Equation for a Simple Pendulum

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Homework Help Overview

The discussion revolves around deriving the time period equation for a simple pendulum, specifically focusing on the differential equation \(\frac{d^2\theta}{dt^2} + \frac{g}{L}\theta = 0\). Participants are exploring the relationship between angular displacement and time, as well as the implications of the general solution involving trigonometric functions.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants discuss the general solution of the differential equation and question the necessity of trigonometric functions in the solution. There are inquiries about the role of constants in the solution and how to apply initial conditions to determine these constants.

Discussion Status

The discussion is ongoing, with participants providing hints and guidance on how to approach the problem. Some have suggested checking the validity of the derived solutions by substituting them back into the original differential equation. There is a recognition of the need to understand initial conditions to fully resolve the constants in the general solution.

Contextual Notes

Participants are working under the constraints of homework guidelines, which may limit the depth of explanations and the provision of complete solutions. There is an emphasis on understanding the derivation process rather than simply obtaining the final equation.

Hootenanny
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I am attempting to derrive the equation for the time period of a simple pendulum, the notes we have been given show some hints to where we should be aiming to get. I have managed to get to
[tex]\frac{d^2\theta}{dt^2} + \frac{g}{L}\theta = 0[/tex]
However, the next line should be
[tex]\theta = \theta_{max} \sin \sqrt{\frac{g}{L}} \theta[/tex]
I've tried intergrating, taking [tex]\theta[/tex] out as a factor and multiplying by [tex]dt^2[/tex] but cannot get the correct solution. Any help would be much appreciated.
 
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The general solution to your ODE is

[tex]\theta (t)=A\sin \omega t +B\cos \omega t[/tex],

where [itex]\omega=\sqrt{\frac{g}{L}}[/itex] and the exact form of the coefficients depends on the 2 initial conditions.

Daniel.
 
I don't unstand why the general solution should contain trig functions are where the [tex]t[/tex] goes.
 
Last edited:
If anyone has the time could they show me a step by step method?
 
Hootenanny said:
I don't unstand why the general solution should contain trig functions are where the [tex]t[/tex] goes.
The differential equation indicates you want that the sum of a function and its second derivative to be zero (aside from the g/L factor that can be normalized out). The trig functions sin and cos have exactly this property. You seem to be wanting to derive the solution simply by manipulating the equation. It's not that simple. Welcome to the wonderful world of differential equations.
 
Hootenanny said:
I don't unstand why the general solution should contain trig functions are where the [tex]t[/tex] goes.
By studying the differential equation, you will realize that the solution must be a function whose 2nd derivative is proportional (within a constant) to the function itself. Trig functions satisfy that requirement. (This might help a bit: http://hyperphysics.phy-astr.gsu.edu/hbase/pend.html#c3)
 
So where do I go from [tex]\theta (t)=A\sin \omega t +B\cos \omega t[/tex]? Do I just sub it in for theta?
 
Right! If it works, then how could it be wrong? You will find directly that it works provided [itex]\omega=\sqrt{\frac{g}{L}}[/itex].
 
  • #10
Do I have to prove that [tex]\omega=\sqrt{\frac{g}{L}}[/tex] or can I just state it?
 
  • #11
Do I just leave the A and B in or do I have to sub something in for them?
 
  • #12
Hootenanny said:
Do I have to prove that [tex]\omega=\sqrt{\frac{g}{L}}[/tex] or can I just state it?
Did you actually try the solution? Did you plug it into the differential equation? It will be pretty obvious what happens and why omega MUST satisfy [itex]\omega=\sqrt{\frac{g}{L}}[/itex].

Re A and B, these are just the amplitude. You can equally well write the solution as
[tex]\theta (t)=A\sin (\omega t +\phi)[/tex]
Where A is theta_max and phi is another constant. You can determine the constants by the initial conditions: What is theta at t=0? What is the speed of the bob (Ld theta/dt) at t=0?
 
  • #13
Yeah I did, but messed it up and couldn't get it to work. I'm going to try again now.
 
  • #14
After manipulating I got [tex]\frac{g}{L}\theta - \omega^2 A\sin (\omega t + \phi ) = 0[/tex] I think its correct.
 
Last edited:
  • #15
Ive got [tex]\frac{g}{L}\theta = \omega^2 A\sin (\omega t + \phi )[/tex] but i don't know how to now prove that [itex]\omega=\sqrt{\frac{g}{L}}[/itex] Help Please.
 
  • #16
What is theta equal to? Look at my last equation in Post #12. I don't know how you fail to see the cancellation.
 
  • #17
O dear, it's been staring me in the face! I can't believe I missed it! Sorry. Thank's for all you help.
 
  • #18
Now I have [tex]\theta = \theta_{max} \sin(\sqrt{\frac{g}{L}} t - \alpha )[/tex] How Can I remove the [itex]\alpha[/itex] ?
 
Last edited:
  • #19
bumping thread
 
  • #20
If theta=0 at t=0, then what must alpha be? If theta=theta_max at t=0, then what must alpha be? This is what is meant by "initial conditions". For a second order differential equation like you started with, the general solution will have two arbitrary constants. In your chosen form of the general solution, these are theta_max and alpha. These can be uniquely determined if you know the initial conditions.
 
  • #21
Ok thanks very much.
 

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