This page builds every symbol in the parent note from absolute zero. If a word or squiggle appeared there without explanation, it gets explained here — in the order that lets each idea rest on the one before it.
The picture: imagine a 1m×1m×1m box of air. Weigh it — about 1.23kg at sea level. That number isρ for air.
Why the topic needs it: to be pushed sideways, air must have mass. Heavier air (bigger ρ) means more momentum to deflect, so more lift. That is why a plane climbs harder to thin, high-altitude air where ρ drops.
The picture (figure above): the wing sits in a river of parallel arrows all pointing the same way with the same length — that uniform flow is V∞. Near the wing the arrows bend and change length; far away they are all identical again.
Why two names for speed? Because near the wing the air speeds up and slows down. We need a fixed reference — the undisturbed speed V∞ — to compare against. (See Bernoulli's Principle for what speed changes do.)
The picture (figure above): the loop C is a dashed ring around the airfoil. At each point sits a short amber arrow dl tangent to the ring, and a cyan arrow V showing which way the air actually moves there.
Why we need this: we are about to measure the swirl. To do that we walk all the way around and ask, at every step, "is the air helping me walk this way, or fighting me?" Each step contributes a little bit, and dl is that little step.
Why the topic needs it: swirl means the air flows around the loop — mostly with your walk. Adding up all these "with/against" numbers is exactly how we score the swirl.
The picture (figure above): on the top leg of the loop the air (cyan) and your walk direction (amber) roughly agree → positive contributions. On the bottom leg they oppose → also adds to a net one-way swirl. Add every step and you get one number, Γ.
Recall What does each piece of
∮CV⋅dl mean?
∮C ::: sum continuously around the whole closed loop CV⋅dl ::: at each tiny step, how much the air flows with your walk
the total ::: Γ, the net swirl of air around the wing
The picture: arrows pushing inward on the wing from below (strong, high p) and from above (weak, low p). The mismatch is a net upward shove.
Why the topic needs it: lift is this net push. And Bernoulli's Principle links it to speed: faster air ⇒ lower pressure. Fast top + slow bottom ⇒ low top pressure + high bottom pressure ⇒ upward Δp.
The picture: the wind arrows come in horizontally; the wing is tilted up by a small wedge angle α from that horizontal. Bigger tilt ⇒ more air deflected ⇒ more swirl ⇒ more lift, up to a point.
Why the topic needs it: for a thin wing, Thin Airfoil Theory gives Γ=πV∞cα — the swirl grows straight in proportion to the tilt. This links a geometric control (how much you point up) to the swirl that makes lift.