By mapping the integrated 𝜌 of each 𝑑GB ! (𝜃, 𝜙) to its corresponding position at 𝑆 ! (𝜃, 𝜙), we produce the gradient bundle condensed charge density, 𝒫 ! (𝜃, 𝜙), which has units of electrons per angular area, specifically electrons per steradian (𝑠𝑟). Additionally, for any atomic scalar property field, 𝐹 ! , there exists a corresponding gradient bundle condensed scalar field, ℱ ! , that is a function of 𝜃 and 𝜙 and a functional of 𝐹 ! , such that, 4 Surfaces through which the flux of ∇𝜌 is everywhere zero, i.e. ∇𝜌 is everywhere tangent to the surface. There also exist net zero flux surfaces whose total, integrated gradient flux is zero.