So let’s put the constant back in And now once again rearrange to get it in a nicer looking form, We’re nearly there now. Those two derivatives are maybe-- for some funny Hamiltonians, you can have even more than two derivatives or more complicated things. Thus we get the relation we needed for I: \begin{equation} \label{Eq:I:47:9} \rho_e = -\rho_0\,\ddp{\chi}{x}.\quad\text{(I)} \end{equation} This equation is what we would expect physically. Open to major codes PY26, PY28, PY29, PY30, PY31, PY32, PY33, and PY34 only.

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