Equation of motion in harmonic oscillator hamiltonian

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SUMMARY

The discussion focuses on the equations of motion in Hamiltonian mechanics, specifically how the time evolution of position and momentum is derived. The equations are defined as the partial derivatives of the Hamiltonian (H) with respect to momentum (p) and position (x), respectively. The relationship is established through the Poisson bracket, which states that the time derivatives are given by the equations: ˙x^i = {x^i, H} and ˙p_j = {p_j, H}. This fundamental concept is typically covered in introductory Hamiltonian mechanics textbooks within the first ten pages.

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oristo42
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nasLoSv.jpg

See attached photo please.

So, I don't get how equations of motion derived. Why is it that x dot is partial derivative of H in term of p but p dot is negative partial derivative of H in term of x.
 

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oristo42 said:
So, I don't get how equations of motion derived. Why is it that x dot is partial derivative of H in term of p but p dot is negative partial derivative of H in term of x.
This follows from the definition of the Poisson bracket and is the basic definition of equations of motion in Hamiltonian mechanics. Any textbook covering Hamiltonian mechanics should tell you this at most 10 pages after starting the discussion on the subject.

The phase space evolution of a system in canonical coordinates is given by
$$
\dot x^i =\{x^i,H\},\quad \dot p_j = \{p_j, H\}.
$$
Indeed, for any time-independent function ##f## on phase space
$$
\dot f = \{f,H\}.
$$
 

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