Hamiltonian for classical harmonic oscillator

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SUMMARY

The Hamiltonian for a classical harmonic oscillator is expressed as H = ω/2(p² + q²), where H = 1/2 m q̇² + k/2 q², with the relationships mq̇ = p and ω² = k/m. The variables p and q represent momentum and position, respectively, and the time derivative of q is denoted as q̇. To transform the standard form H = (p²/2m) + (1/2)mω²q² into the desired form, one must rescale the variables p and q, a process known as canonical transformations.

PREREQUISITES
  • Understanding of Hamiltonian mechanics
  • Familiarity with classical mechanics concepts such as momentum and position
  • Knowledge of canonical transformations
  • Basic calculus, particularly derivatives
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  • Study Hamiltonian mechanics in-depth
  • Learn about canonical transformations in classical mechanics
  • Explore the derivation of the harmonic oscillator Hamiltonian
  • Investigate the implications of rescaling variables in physical systems
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This discussion is beneficial for physics students, educators, and researchers focusing on classical mechanics, particularly those studying Hamiltonian systems and harmonic oscillators.

Jacksond
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I am working through Leonard Susskinds 'the theoretical minimum' and one of the exercises is to show that H=ω/2(p^2+q^2).

The given equations are H=1/2mq(dot)^2 + k/2q^2, mq(dot)=p and ω^2=k/m.

q is a generalisation of the space variable x, and (dot) is the time derivative if this helps. The solution I am getting contains variables in front of the q and p's inside the brackets, do these reduce somehow? Any proof/explanation would be much appreciated :)
 
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So ##H = \frac{p^2}{2m} + \frac{1}{2}m\omega^2 q^2## is the standard form of the harmonic oscillator Hamiltonian. Now all you have to do is rescale ##p## and ##q## appropriately to get it into the desired form (this rescaling of the conjugate variables is a special case of what are known as canonical transformations).
 

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