(Assuming you haven't already found the answer) From my undergraduate understanding of QM, the energies of electrons' wave functions in an object exert pressure on the walls of the object since fermions can't exist in degenerate states. So in a 1-D or 2-D examples of charged objects, you can't actually approximate to 1-D and 2-D analogs since electrons' wave functions are inherently 3-D.
Sorry, I've been so sporadic these last two weeks. Mid-terms are over for me, so I can find time to work through the book again. Does anyone have a list of problems they think are essential from chpt. 2?