The vector potential and the Hamiltonian?

[jeebs]

Hi,
I have a problem involving the Hamiltonian of a particle of mass m, charge q, position r, momentum p, in an external field defined by vector potential A and scalar potential X. Here's the Hamiltonian:

H(r,p) = (1/2m)[p - qA(r,t)]² + qX(r,t) = (1/2m)(p_jp_j - 2qp_jA_j + q²A_jA_j) + qX

The problem I have to solve is that i have to show that

\dot{A} = \partial _{t} A + (v \bullet \nabla)A

My attempted solution:

When I put this into Hamilton's equations of motion, (which are the following:)

\frac{dr_{j}}{dt} = \frac{\partial H}{\partial p_{j}} and \frac{dp_{j}}{dt} = - \frac{\partial H}{\partial r_{j}}

I get : \ \frac{\partial H}{\partial p_{j}} = (1/m)(p_{j} - qA_{j}) = \frac{dr_{j}}{dt} = v_{j}

and : \ \frac{\partial H}{\partial r_{j}} = (\frac{q^{2}A_{j}}{m} - \frac{qp_{j}}{m})\frac{\partial A_{j}}{\partial r_{j}} + q\frac{\partial X}{\partial r_{j}}= - \frac{dp_{j}}{dt} = F_{j}

I am 99% certain these are correct.



Using what I got for the first differential equation, i find that A_{j}=(1/q)(p_{j} - mv_{j})

hence \ \dot{A} = \frac{1}{q}(\frac{dp_{j}}{dt} - m\frac{dv_{j}}{dt})

\ = \frac{1}{q}((-(\frac{q^2A_{j}}{m} - \frac{qp_{j}}{m})\frac{dA_{j}}{dr_{j}} + q\frac{\partial X}{\partial r_{j}}) - m\frac{dv_{j}}{t})

\ = (\frac{p_{j}}{m} - \frac{qA_{j}}{m})\frac{\partial A_{j}}{\partial r_{j}} - \frac{\partial X}{\partial r_{j}} - m\frac{dv_{j}}{dt})

\ = (v_{j}.\nabla)A_{j} - \frac{\partial X}{\partial r_{j}} - m\frac{dv_{j}}{dt}

and this is as far as I get really.

First off, am I correct in the way i got to the (v.\nabla) part? (ie. using the first Hamilton equation for velocity?)

Assuming that is correct, I haven't been able to find a way to deal with the other terms in the equation... the advice given on the question sheet is to use the chain rule in index notation, but I don't see where this comes in handy for this question.

Can anyone offer any advice on how to tackle this one?

Thanks.

 

[gabbagabbahey]

You're making things much too complicated...A is a function of r_i and t, so the chain rule tells you

\dot{A}=\frac{dA}{dt}=\partial_t A+\frac{dr_i}{dt}\frac{\partial A}{\partial r_i}