Use Gauss's Law to derive electric field formulas for symmetric charge distributions (wire, sheet, shell).
Derivation using a cylindrical Gaussian surface.
Imagine an infinitely long, thin straight wire with a uniform linear charge density . Because the wire is perfectly straight and infinite, it has cylindrical symmetry. This means the electric field must look the same from any angle around the wire and must point radially outward (if ).
Derivations for a sheet and a thin shell.
Consider an infinite flat sheet with a uniform surface charge density . By symmetry, the electric field must point straight away from the sheet (if positive) and cannot depend on your or coordinates along the plane.
Matrix of formulas for wire, sheet, and shell.
Derives field for a uniform spherical charge distribution.
Problem
An early model for an atom considered it to have a positively charged point nucleus of charge , surrounded by a uniform density of negative charge up to a radius . The atom as a whole is neutral. For this model, what is the electric field at a distance from the nucleus?
Calculate linear charge density given the field.
Problem: An infinite line charge produces an electric field of at a distance of . Calculate the linear charge density .
Solution: We know the formula for the electric field of an infinite line charge is . To find the linear charge density, we rearrange the formula to isolate : . Now, we substitute the given values: and . Using the electrostatic constant , we can write . Plugging these into our rearranged equation gives . Calculating this yields the final linear charge density: .
MCQ testing the r-dependence of different fields.
How does the magnitude of the electric field of an infinitely long, uniformly charged wire scale with the radial distance ?