The three-dimensional story so far assumed the wing flies in open air, free to trail its vortex system as deep as it likes. Within roughly a wingspan of the runway that assumption fails: the ground is in the way. The result is ground effect: the aircraft flying measurably better in the last few metres than anywhere else, and every flight passes through it twice (once climbing out, once flaring to land). This lesson explains the mechanism and then follows it into the flare, the lift-off, and the differences a wing's height above the ground makes.
What the ground does to the vortex system
The tip vortices and the downwash they feed need room below and behind the wing to develop. Close to the ground that room is gone: the surface blocks the downward flow, the tip vortices cannot grow to full strength, and the downwash at the wing is reduced. The whole airflow pattern flattens: streamlines that would have been deflected steeply downward now leave the wing more nearly horizontally, with a region of raised pressure beneath, often called a cushion, though it is not air compressed under the wing: the mechanism is the vortex system being suppressed.
Now replay the induced-drag lesson with a weaker downwash. Less downwash means a smaller induced angle of attack, so the effective airflow is less tilted, the lift vector leans back less, and the induced drag coefficient falls: at the same geometric angle of attack the wing produces more lift and less drag. The effect switches on gradually with height: barely noticeable at one wingspan above the surface, clear below half a wingspan, and strong in the flare: at a height of about a tenth of the span, the induced drag coefficient can be roughly halved.