Average kinetic energy of a damped oscillator

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SUMMARY

The average kinetic energy of a damped mechanical oscillator is defined by the equation $$E = \frac{1}{2}m \dot{x}^2 + \frac{1}{2}k x^2$$, where ##k## represents the spring constant. It is established that the average kinetic energy, denoted as ##\langle T \rangle##, is half of the total energy of the system. This relationship is derived from the oscillatory nature of energy transfer between kinetic and potential forms. A formal approach to demonstrate this involves calculating the average value of a function over a specified interval using the formula $$y_{avg}=\frac{1}{b-a}\int_a^b f(x)\;\text{d}x$$.

PREREQUISITES
  • Understanding of mechanical oscillators and damping
  • Familiarity with the concepts of kinetic and potential energy
  • Knowledge of calculus, specifically integration
  • Basic grasp of harmonic motion and spring constants
NEXT STEPS
  • Explore the derivation of energy conservation in damped oscillators
  • Study the mathematical implications of the average value theorem in physics
  • Learn about the effects of damping on oscillatory systems
  • Investigate the relationship between energy transfer and oscillation frequency
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Students of physics, mechanical engineers, and anyone studying the dynamics of damped oscillatory systems will benefit from this discussion.

MuIotaTau
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For a damped mechanical oscillator, the energy of the system is given by $$E = \frac{1}{2}m \dot{x}^2 + \frac{1}{2}k x^2$$ where ##k## is the spring constant. From there, I've seen it dictated that the average kinetic energy ##\langle T \rangle ## is half of the total energy of the system. This makes sense, since the energy sort of "sloshes" back and forth between kinetic and potential energy, but is there a more formal way to show this is true?
 
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if you have ##y=f(x)## then the average value of ##y## in ##a<x<b## is the height of a rectangle with the same area as the graph of ##y## vs ##x## in that region. $$y_{avg}=\frac{1}{b-a}\int_a^b f(x)\;\text{d}x$$
 
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Oh, that's simple! Thank you!
 

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