Hamiltonian
@Michele_Laino
Ok so my question is, when you get to the end of the problems and need to find the equation of motions we use \[\huge \dot{q_i} = \frac{ \partial H}{ \partial P_i }~~~~P_i = - \frac{ \partial H }{ \partial q_i }\] right
So when you find these is that the final solution or do we still have to take the time derivative of these and add them up to get the final equation of motion?
you have to take the derivative of H with respect to q_i and p_i respectively, and then you have to integrate them with respect to time
so you will get the functions q_i and p_i
Oh right because that should P_i dot there right, which then gives you P_i and q_i
So once you integrate it, do you just add the two functions or leave them be?
yes! The hamiltonian equations are: \[\large \begin{gathered} \dot q = \frac{{\partial H}}{{\partial p}} \hfill \\ \dot p = - \frac{{\partial H}}{{\partial q}} \hfill \\ \end{gathered} \]
Oh wait so we integrate it as \[\int\limits \dot{P_i} dt\]
yes!
similarly for \[{\dot q}\]
Oh I kept thinking we integrate it as \[\int\limits \dot{p_i} di\] haha
:)
So once the integrate is done, that will be our equation of motion right, mhm interesting, it's hard to tell sometimes without units xD.
yes! please keep in mind that the functions q and p are important in statistical physics
Mhm ok weird in my notes I have an example that is integrated \[\int\limits \dot{P_i} di \]
I think it is a typo error, since i is only an index which runs over the degrees of freedom of our mechanical system
So it shows \[\dot{P_y} = - \frac{ \partial H }{ \partial y } = - mg \implies P_y = - mgy+C\]
please wait...
No problem
\[\large {p_y} = -\int {mg} \;dt\]
Yes that would be -mgt+C no?
yes!
Mhm wonder why there's a y.
since you have found H
\[\large H = mgy + f(x,t)\]
since, in general H= H(x,y,t)
Oooh ok, thanks :)
thanks! :)
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