Coordinate Systems and the Differential Element
Match the differential cell to the chunk of space
Drag to inspect the golden chunk of space. Which coordinate system tiles it with no gaps?
Cartesian — a straight cube
The three axes are mutually perpendicular with uniform spacing everywhere. The differential volume is just the product of three edges. No curved edge, so every scale factor is 1.
Cylindrical — an angle becomes an arc
The larger ρ is, the more distance the same angle dφ sweeps. So the φ-edge has length ρ dφ, not dφ. The ρ that turns an angle into a length is the scale factor.
Spherical — two arcs
The meridian edge is an arc on a circle of radius r, so r dθ. The parallel edge rides a smaller circle of radius r sinθ, not r, so r sinθ dφ. The two scale factors multiply into r² sinθ.
Surface elements follow the same logic
A patch on a sphere of radius r has area equal to the product of two arcs: dA = r² sinθ dθ dφ. The Gauss-law surface integral in the next units is exactly the summing of these patches.
Back to the first screen
What filled the golden chunk with no gaps was the spherical differential cell. Its three edges (dr, r dθ, r sinθ dφ) grow along the same directions as the chunk’s symmetry. The cube could not follow the curved surface, and the cylindrical wedge mismatched at top and bottom. Choosing a coordinate system is, in the end, shaping the differential cell to the symmetry of the problem.
Coordinate systems and differential elements are the handle for every field integral. Once you equip this tool, the next units open up: scalar and vector fields (EM-02), electric flux and divergence (EM-05), and the Gauss-law surface integral (EM-06) all happen on the differential cell you choose here.