Period and probability density for a harmonic oscillator

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Printed solution to a classical harmonic oscillator problem: energy E = (k/2)l^2 = (k/2)x^2 + (m/2)x^2, period T = 2 times the integral from -l to l of dx over sqrt((2E - kx^2)/m) = 2 pi sqrt(m/k), and p(x) = (1/pi)(k/(2E - kx^2))^(1/2).

##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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  • Printed solution to a classical harmonic oscillator problem: energy E = (k/2)l^2 = (k/2)x^2 + (m/2)x^2, period T = 2 times the integral from -l to l of dx over sqrt((2E - kx^2)/m) = 2 pi sqrt(m/k), and p(x) = (1/pi)(k/(2E - kx^2))^(1/2).
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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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