The figure below draws one such address on a flat xy-sheet: the yellow dot sits at x=3.5, y=2.5, and the blue dashed lines show how each coordinate is measured off its axis. Whenever this page says "a point", picture that yellow dot.
Why the topic needs it: curl is a local measurement — it lives at one point. Before we can say "the spin here" we need a way to name "here". That name is (x,y,z).
Why the topic needs it: the thing curl acts on is a flow, and a flow at a point is exactly "an arrow saying which way and how fast the water moves there". That arrow is a vector.
The figure shows the field F=(−y,x,0): a whole grid of blue arrows, one per point. Follow the yellow dot at (1,0) — its arrow points straight up — and the pink dot at (0,1) — its arrow points left. Sweep your eye around the origin and the arrows chase each other counterclockwise, the whirlpool described just below.
Why the topic needs it: curl compares the arrow here with the arrows just next door. That comparison only makes sense if there's an arrow at every neighbouring point — i.e. a field, not a single vector.
Why this tool and not another? Curl asks "does the flow on the bottom of the wheel differ from the flow on the top?" — a difference across a direction. A partial derivative is precisely the tool that measures "how much does the field differ as I move a tiny bit in one direction". No other tool answers that question as cleanly.
Why the topic needs it: the parent's core formula divides circulation by the area A=ΔxΔy then shrinks the loop. Without the small steps Δx,Δy,Δz (to build the loop and its area) and lim (to shrink it) that sentence is meaningless.
The three little arrow-pairs in the figure make this concrete: yellow and blue nearly aligned (top-left) → big positive; at right angles (top-right) → zero; pointing against each other (bottom) → negative.
Why the topic needs it: circulation is ∮F⋅dr. Along each edge of the paddlewheel loop we ask "how much of the flow F points along the way I'm walkingdr?" That's a dot product. If flow and walk agree it adds to the spin; if perpendicular it contributes nothing.
The figure shows this pairing: blue arrows run counterclockwise around the loop, and the yellow axle points straight out of the board — thumb-and-fingers of the right hand.
Why the topic needs it: this integral — with its orientation nailed down — is the definition of curl in the limit: circulation per area, sign fixed by the right-hand rule. It is the beating heart of the parent note.
Why the topic needs it: the parent's identity ∇×(∇ϕ)=0 is entirely this fact — the two mixed partials cancel. See Equality of Mixed Partial Derivatives (Clairaut) and Gradient and Conservative Fields.
Read it as: locations build arrows, arrows build fields, fields plus partial derivatives build both circulation (via dot product and loop) and an axis (via cross product) — and those two meet to become curl.