An infinite plane slab of uniform volume charge density occupies the region with ;…

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

An infinite plane slab of uniform volume charge density ρ0=2.0×10−6 C m−3\rho_0 = 2.0\times10^{-6}\,\mathrm{C\,m^{-3}} occupies the region −t≤z≤t-t \le z \le t with t=3.0 mmt = 3.0\,\mathrm{mm}; outside the slab there is vacuum. By symmetry VV depends only on zz. Inside the slab it is proposed that V(z)=V0−ρ02ε0z2,∣z∣≤t,V(z) = V_0 - \frac{\rho_0}{2\varepsilon_0}z^2, \qquad |z|\le t, with V0V_0 a constant, and outside the slab (for z>tz>t) that V(z)=A−BzV(z) = A - Bz for constants AA, BB. ((a)) Show that the proposed inside form satisfies Poisson's equation with source ρ0\rho_0. ((b)) Show that the proposed outside form satisfies Laplace's equation, and find the constant BB by requiring dV/dzdV/dz (hence the field) to be continuous at z=tz=t, where there is no surface charge.

Browse the problem library