A parallel-plate capacitor in vacuum has plates of area

PHYSICS · Multi-part · Fermi University Physics · Electricity, Magnetism & Electromagnetism · Conductors, capacitance and boundary-value electrostatics · Conductors, capacitance and boundary-value electrostatics

The Boundary-Value Problem, Ch The field as a differential equation: Poisson, Laplace and the well-posed problem

Problem

A parallel-plate capacitor in vacuum has plates of area A=2.0×10−2 m2A = 2.0\times10^{-2}\,\mathrm{m^2}, separated by d=1.0 mmd = 1.0\,\mathrm{mm}, with edge effects ignored so VV depends only on the coordinate zz between the plates (0≤z≤d0\le z\le d). The plate at z=0z=0 is earthed. The plate at z=dz=d is isolated, not connected to any battery, and carries a fixed free charge Qfree=5.0 nCQ_{\rm free} = 5.0\,\mathrm{nC}. Neglect the field outside the plates, so that all of QfreeQ_{\rm free} sits on the top plate's lower face, the face that looks into the gap. ((a)) Write down the region Ω\Omega, the equation holding inside it, and the data on each plate (z=0z=0 and z=dz=d). ((b)) Classify the two pieces of boundary data (Dirichlet, Neumann, or the third, known-charge kind), and say whether the overall problem is Dirichlet, Neumann or mixed.

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