Please help explain the probability density function

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SUMMARY

The discussion focuses on the derivation and understanding of the probability density function (PDF) in the context of classical mechanics, specifically for a harmonic oscillator. The key equations presented include the energy equation, \(E = \frac{1}{2}(kx^2 + m \dot{x}^2)\), and the relationship between time and position, \(dt = \sqrt{\frac{m}{2E - kx^2}}dx\). The user seeks clarification on why the PDF is defined as \(p(x) = \frac{2dt}{T}\), where \(T = 2\pi\sqrt{\frac{m}{k}}\) represents the period of oscillation. The discussion emphasizes the connection between the time spent in an interval and the probability of finding the oscillator in that interval.

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  • Understanding of classical mechanics, particularly harmonic motion
  • Familiarity with the concepts of energy conservation and kinetic/potential energy
  • Knowledge of calculus, specifically integration and differentiation
  • Basic understanding of probability theory and probability density functions
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##E = \frac{1}{2}(kx^2+m \dot{x}^2)##
## \frac{2E - kx^2}{m}=\dot{x}^2##
##\frac{dx}{dt} = \sqrt{\frac{2E - kx^2}{m}}## or ## dt = \sqrt{\frac{m}{2E - kx^2}}dx ## ⇒##= \frac{1}{\sqrt{\frac{2E - kx^2}{m}}}dx##

My Question please help me.
1. I know ##T = 2\pi\sqrt{\frac{m}{k}} .## but i don't understand why ##T = 2 \int_{-l}^{l}\frac{1}{\sqrt{\frac{2E - kx^2}{m}}}dx##2.In this case. Why do we choose the probability density function, ## p(x) = \frac{2dt}{T} ## ?
 

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I don't understand how to define the probability density function.
 
1. The denominator is the speed at position x (see the equation for E). The time dt spent in the interval dx is dx/vx.
2. The probability of being between x and x+dx equals the fraction of the time that is spent in this interval, i.e. 2dt/T (2 because it traverses this interval twice in a full period), where dt is related to dx as above.
 
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