Stall speed and the polar
Both families raise CLmax, so both cut the stalling speed: the square-root relation from the previous lesson does not care where on the chord the extra lift was found. And a lower stalling speed is runway arithmetic: rotation, lift-off and approach speeds all scale down with it, so the take-off run and the landing distance shorten. The comparison the exam wants: a trailing-edge flap, especially a Fowler, delivers the larger rise in maximum lift coefficient and therefore the larger stall-speed reduction; a leading-edge device alone adds less. But the leading-edge device collects its gain at a far smaller drag price. On the polar, a deployed slat barely moves the curve to the right: it mostly extends it upward, to lift coefficients the clean polar never reached. The maximum CL/CD consequently suffers far less than with trailing-edge flap. That low drag price is why take-off configurations lean on the leading edge: lift for the runway without a heavy drag penalty in the climb that follows. And it is why the two families are fitted together: the flap providing the lift and the flat attitude, the slat pushing the stalling angle back up, keeping the stall a safe margin above the angles actually flown.
The attitude price
The leading-edge device's weakness is where its benefit lives: at high angles of attack. A wing relying on slats for its landing lift must be flown at the steep angles where the slat actually delivers its benefit, and with the flight path fixed on the glide slope, more angle of attack means more nose-up pitch attitude. The disadvantages mirror the flap's advantages from the previous lesson: the nose blocks the view of the runway, the tail swings closer to the surface, and the margin to a tailstrike in the flare shrinks. This is the other half of why no transport wing relies on slats alone for landing: the trailing-edge flap pulls the required angle of attack (and with it the attitude) back down, while the slat keeps the stall safely above it.
Slat asymmetry
Asymmetric slats are treated with the same severity as asymmetric flaps, and near the stall they are worse. At ordinary angles of attack a deployed slat changes little, so the asymmetric pair flies deceptively normally. The danger surfaces at high angle of attack: the slatted wing keeps flying to its raised critical angle while the clean wing stalls at its own, lower one: one wing stalls, the other does not. The result is a sudden, powerful rolling moment toward the stalled wing, at low speed, close to the ground, where aileron authority is least and may be insufficient. As with flaps, the system's answer is prevention: slat positions are monitored, and a detected asymmetry freezes the system before the difference can grow.
Vortex generators
The last device is small enough to miss on a walkaround: vortex generators: rows of little vanes, each a few centimetres tall, standing on the upper surface. Each vane is a tiny wing set at an angle to the local flow, and like any lifting wing it sheds a tip vortex. That vortex is the tool. Spinning downstream, it stirs the layers of air together: fast, energetic air from just above the boundary layer is mixed down into the slow layer at the surface. The boundary layer downstream of the row is re-energised, exactly as with the slot, and stays attached at angles where it would otherwise have separated. The purpose is therefore to delay flow separation over whatever lies behind the row: an aileron that must keep biting at high angle of attack, a wing region prone to letting go early, or (on fast wings) the separation behind a shock wave, which is the high-speed module's business.