Time averages for a 2-dimensional harmonic oscillator

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SUMMARY

This discussion focuses on calculating time averages for a two-dimensional classical harmonic oscillator in the context of Ergodic Theory. The kinetic energy is defined as $$T=\frac{\dot x^2}{2}+\frac{\dot y^2}{2}$$ and the potential energy as $$U=\frac{x^2}{2}+\frac{y^2}{2}$$. The time average of the potential energy is given by $$\langle U \rangle=\frac{1}{T} \int_0^T \mathrm{d} t \frac{1}{2} (x^2+y^2)$$, where ##T## represents the period of motion. The discussion confirms that the time averages in two dimensions are qualitatively similar to those in one dimension.

PREREQUISITES
  • Understanding of classical mechanics, specifically harmonic oscillators.
  • Familiarity with Ergodic Theory concepts.
  • Knowledge of integral calculus for calculating time averages.
  • Ability to solve differential equations of motion for oscillatory systems.
NEXT STEPS
  • Study the derivation of the equations of motion for a two-dimensional harmonic oscillator.
  • Learn about the implications of Ergodic Theory in classical mechanics.
  • Explore the calculation of time averages in multi-dimensional systems.
  • Investigate the differences between one-dimensional and two-dimensional harmonic oscillators.
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Students and researchers in physics, particularly those focusing on classical mechanics and Ergodic Theory, as well as anyone interested in the mathematical treatment of harmonic oscillators.

Lo Scrondo
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I'm studying Ergodic Theory and I think I "got" the concept, but I need an example to verify it...

Let's take the simplest possible 2D classical harmonic oscillator whose kinetic energy is $$T=\frac{\dot x^2}{2}+\frac{\dot y^2}{2}$$ and potential energy is $$U=\frac{ x^2}{2}+\frac{y^2}{2}$$.

I'd like to find the time averages of the two quantities. My intuition is that they arent't qualitatively different from the one-dimensional case, but I'd really welcome some help
 
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You'll find that the oscillator has harmonic solutions and then the time average is
$$\langle U \rangle=\frac{1}{T} \int_0^T \mathrm{d} t \frac{1}{2} (x^2+y^2),$$
where ##T## is the period of the harmonic motion, and analogously for the kinetic energy.

So just write down the general solution of your equations of motion and calculate the integrals. It's not too difficult.
 

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