Rotating a vector 90° then pushing it through f must match pushing first then rotating – otherwise the map isn’t complex-differentiable.
These grids make that concrete: the top shows df(zX) while the bottom shows z·df(X); forcing them equal unpacks straight into the Cauchy-Riemann pair
∂u/∂x = ∂v/∂y
∂u/∂y = −∂v/∂x.
Aircraft engineers lean on exactly these relations when they build conformal maps to forecast airflow over wing sections, skipping full Navier-Stokes runs for early design loops.
Which single arrow in the picture finally made the two equations feel inevitable to you?