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I recently searched up the definition for a more generalized definition of charge whether it be color charge or electric charge . And I found this but i fail to understand what this statement actually means :

A charge is any generator of a continuous symmetry of the physical system under study. When a physical system has a symmetry of some sort, Noether's theorem implies the existence of a conserved current. The thing that "flows" in the current is the "charge", the charge is the generator of the (local) symmetry group. This charge is sometimes called the Noether charge.--- Source Wikipedia

Taking this statement " A charge is any generator of a continuous symmetry of the physical system under study."

What do continuous symmetry means and generator mean? How does a charge create a continuous symmetry and how does it impact the physical system?

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  • $\begingroup$ You should search up principle of least action and lagrangian first. Try to get your hands on David morins classical mechanics book. $\endgroup$ Commented Aug 19, 2022 at 10:54
  • $\begingroup$ Exactly what part of lagrangian mechanics can help on the understanding of this ? $\endgroup$ Commented Aug 19, 2022 at 10:58
  • $\begingroup$ Maybe this helps you $\endgroup$ Commented Aug 19, 2022 at 11:13
  • $\begingroup$ Quote from which Wiki page? $\endgroup$
    – Qmechanic
    Commented Aug 19, 2022 at 11:50
  • $\begingroup$ en.wikipedia.org/wiki/Charge_(physics) - for your reference $\endgroup$ Commented Aug 20, 2022 at 5:21

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  1. OP's question is related to the converse/inverse Noether's theorem, cf. e.g. this Phys.SE post.

  2. Let us for simplicity only consider the Hamiltonian formulation. In the Hamiltonian formulation a constant of motion/conserved quantity/charge $Q(q,p,t)$ is the generator of a Hamiltonian vector field $X_Q$, which in turn generates a finite continuous Hamiltonian flow. The corresponding infinitesimal transformation is $$\delta z^I ~=~\epsilon\{z^I, Q\}, \qquad I~\in~\{1,\ldots, 2n\}, \qquad \delta t ~=~0,\tag{A}$$ where $\epsilon$ is an infinitesimal parameter. One may show that this is a symmetry of the Hamiltonian action, cf. statement 3 in my Phys.SE answer here.

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