What is the Hamilton-Jacobi equation

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The Hamilton-Jacobi equation reformulates classical mechanics using a function S, which represents action and is useful for separating variables and expressing constants of motion. It relates canonical momenta to the generating function S through partial derivatives, leading to the equation ∂S/∂t + H = 0. An example illustrates its application to the central-force problem, demonstrating how to derive S from the Hamiltonian. The equation shows explicit dependence on the radial coordinate r, suggesting a decomposition of S using energy and angular momentum constants. Overall, the Hamilton-Jacobi equation provides a powerful tool for solving mechanical problems in classical physics.
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Definition/Summary

The Hamilton-Jacobi equation is an additional reformulation of classical mechanics, one that uses a function S variously called the action, the generating function, and Hamilton's principal function.

It is very convenient for problems where one can separate the variables, and it is also convenient for expressing constants of the motion.

Equations

The generating function S is a function of canonical coordinates q_a(t) and constants of the motion \alpha_a. The canonical momenta p_a(t) are given in terms of it by
p_a = \frac{\partial S}{\partial q_a}

and some additional constants of the motion \beta_a by:
\beta_a = \frac{\partial S}{\partial \alpha_a}

Plugging these canonical-momentum values into the Hamiltonian, we find the Hamilton-Jacobi equation:
\frac{\partial S}{\partial t} + H = 0

Extended explanation

To demonstrate what the Hamilton-Jacobi equation can be used for, here is a solution of the central-force problem with potential V(r) using it, complete with separation of variables. We start out with its Lagrangian
L = \frac12 m \left[ \left( \frac{dr}{dt} \right)^2 + r^2 \left( \frac{d\theta}{dt} \right)^2 \right] - V
Its canonical momenta are
p_r = m \frac{dr}{dt}

and
p_\theta = m r^2 \frac{d\theta}{dt}

and thus its Hamiltonian is
H = \frac{(p_r)^2}{2m} + \frac{(p_\theta)^2}{2mr^2} + V

The Hamilton-Jacobi equation becomes
\frac{\partial S}{\partial t} + \frac{1}{2m}\left( \frac{\partial S}{\partial r} \right)^2 + \frac{1}{2mr^2}\left( \frac{\partial S}{\partial \theta} \right)^2 + V = 0

Aside from the partial derivatives, this equation has explicit dependence only on r. This suggests a decomposition of S using constants of the motion E (energy) and L (angular momentum):
S = - Et + L\theta + S'(E,L,r)

We easily find S' from it:
S' = \int \left[ 2m(E - V) - \left( \frac{L}{r} \right)^2 \right]^{1/2} dr

and the remaining constants of the motion, which are zero points:
-t_0 = - t + \frac{\partial S'}{\partial E}
\theta_0 = \theta + \frac{\partial S'}{\partial L}

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This is a great explanation of the Hamilton-Jacobi equation. As someone with no prior knowledge of the subject, I can easily understand what it is used for and how the equation works. Thanks for providing this comprehensive overview!
 
So I know that electrons are fundamental, there's no 'material' that makes them up, it's like talking about a colour itself rather than a car or a flower. Now protons and neutrons and quarks and whatever other stuff is there fundamentally, I want someone to kind of teach me these, I have a lot of questions that books might not give the answer in the way I understand. Thanks
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