There’s more than just differential topology going on, but it’s the thing that unifies it all. You can think of differential topology as being about spaces you can divide into cells, and the boundaries of those cells. Conservation laws are naturally expressed here as constraints that the net flow across the boundary must be zero. This makes conserved quantities into resources, for which the use of is convergently minimized. Minimal structures with certain constraints are thus led to forming the same network-like shapes, obeying the same sorts of laws. (See chapter 3 of Grady’s Discrete Calculus for details of how this works in the electric circuit case.)
There’s more than just differential topology going on, but it’s the thing that unifies it all. You can think of differential topology as being about spaces you can divide into cells, and the boundaries of those cells. Conservation laws are naturally expressed here as constraints that the net flow across the boundary must be zero. This makes conserved quantities into resources, for which the use of is convergently minimized. Minimal structures with certain constraints are thus led to forming the same network-like shapes, obeying the same sorts of laws. (See chapter 3 of Grady’s Discrete Calculus for details of how this works in the electric circuit case.)