Hamiltonian Math: Understanding p-dot and q-dot Terms

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The discussion centers on the differentiation of a generic function G with respect to variables p and q in the context of Hamiltonian mechanics. The terms p-dot and q-dot represent the time derivatives of p and q, respectively, and are essential for applying the chain rule in the differentiation process. The equation $$\frac{dG(p,q)}{dt} = \frac{\partial G}{\partial p} \frac{dp}{dt} + \frac{\partial G}{\partial q} \frac{dq}{dt}$$ illustrates how these terms arise when considering the total derivative of G with respect to time.

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I'm watching a lecture on the Hamiltonian and can't figure out something. Here it is. Take a generic function G, and differentiate it with respect to p and q. What you get is the partial of G with respect to p TIMES the derivative of p (or p-dot), plus the derivative of G with respect to q TIMES q-dot.

My question is, where does the p-dot and q-dot terms come into the equation here? Why isn't it just the partial of G over p plus the partial of G over q?
 
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What you've described looks like taking the derivative of G(p,q) with respect to t, using the chain rule:

$$\frac{dG(p,q)}{dt} = \frac{\partial G}{\partial p} \frac{dp}{dt} + \frac{\partial G}{\partial q} \frac{dq}{dt}$$
 
It certainly does, thanks jtbell.
 

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