What are the simple modes and frequencies for weakly coupled oscillators?

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SUMMARY

The discussion focuses on the oscillatory energy exchange between two coupled simple pendulums of equal length (L = 1m) connected by a spring with a spring constant (K = 0.05 Mg/L). The oscillation behavior is characterized by a "beat" frequency, where the amplitude of one pendulum reaches its maximum when the other reaches its minimum. The period of energy transfer is inversely proportional to the coupling spring constant, with specific equations derived for the maximum amplitudes of both pendulums. The conversation also touches on the potential for asymmetric motion and the existence of simple modes with no energy transfer.

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  • Understanding of simple harmonic motion and pendulum dynamics
  • Familiarity with spring constants and their effects on oscillatory systems
  • Knowledge of differential equations and Lagrangian mechanics
  • Concept of energy conservation in mechanical systems
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Homework Statement


Two simple pendulums os equal length L=1m are connected with spring with a spring constant K=0,05 Mg/L. The pendulums are started by realeasing one of them from a displaced position. The subsequent motion is characterized by an oscillatory energy exchange between the pendulums. What is te period of this transfer?

Homework Equations

The Attempt at a Solution


In this situation, as a pendulum is displaced and the another is static, I suppose that when the amplitude of pendulum 1 is a maximum, the amplitude of pendulum 2 is minimum, because the result is displaying "beat" frequency. That's correct?
 
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Yes. Why ask ?
 
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Yes. When the amplitude of one of the pendula is zero, the amplitude of the other is maximal. This follows directly from energy conservation.
 
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Well, just to get rid of the doubt.

Them, starting from the equation of position, and I found that the maximum values of the amplitude for the pendulum 1 occurs when:

επ(t/T) = nπ ---> t/T = n/ε

The time between maxima is T/ε, inversely proportional to the coupling spring constant.

And for the pendulum 2 when:

επ(t/T) = (2n +1)* π/2 ---> t/T = (2n+1)/2ε

Them, I stuck in here. Can I relate that with period of transfer in the oscillatory energy exchange in some way?
 
Good. So what's this exercise ? In a chapter on differential equations, on Larangian mechanics, a lab instruction preparation perhaps ?

The motion described is asymmetric and one can expect the pendulum that's initially immobile to start swingning too.
There are simple modes possible where there is no transfer; can you guess which ? Wht are their frequencies ?
 

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