Tiny bubbles readily
stick onto substrates owing to contact angle
hysteresis (CAH). Nevertheless, they can slide slowly on a tilted
surface with ultralow CAH because capillarity is overcome by buoyancy.
It is surprising to observe experimentally that bubbles of 3–15
μL (diameter 1.79–3.06 mm) slide beneath a tilted superhydrophobic
surface at a vertical ascent rate faster than that of freely rising
ones of high Reynold numbers ≈O(102). As the tilting angle increases, the drag coefficient remains essentially
the same as that of a freely rising bubble, but the frontal area of
the flat bubble rises monotonically. Nonetheless, the frontal area
of the sliding bubble always stays much smaller than that of a freely
rising bubble. Consequently, the small drag force associated with
the sliding bubbles is attributed to their substantially small frontal
areas on superhydrophobic surfaces.