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Physics LibreTexts

6.8: Hamilton’s Equations

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Having finally established that we can write, for an incremental change along the dynamical path of the system in phase space,

dH(qi,pi)=i˙pidqi+i˙qidpi

we have immediately the so-called canonical form of Hamilton’s equations of motion:

Hpi=˙qiHqi=˙pi

Evidently going from state space to phase space has replaced the second order Euler-Lagrange equations with this equivalent set of pairs of first order equations.


This page titled 6.8: Hamilton’s Equations is shared under a not declared license and was authored, remixed, and/or curated by Michael Fowler.

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