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When a liquid drop is placed on a surface that is held at a temperature much higher than the liquid's boiling point (such as a drop of water in a very hot pan) it hovers on its own vapour cushion, without wetting the surface (figure a below).This phenomenon is called the Leidenfrost effect (or film boiling) and occurs beyond a surface temperature called the Leidenfrost point (about 200 - 300 C for water on flat surfaces, depending on surface quality).

We discovered that film-boiling droplets move at speeds of several centimeters per second when placed on asymmetrically structured surfaces (movie), such as a piece of brass with periodic, saw-tooth shaped ridges (see highspeed movie).

We think that the reason this works is that the ratchet redirects the vapor flow underneath the droplet, so that most of it goes in one direction (figure b below. The droplet the rides along ontop of the vapor, like a boat on a river - one that can flow uphill!

Film-boiling droplets. (a) Cartoon of a film-boiling droplet on a flat surface. The vapour cushion separating liquid and solid is typically 10 - 100 µm thick. (b) Film-boiling droplets on saw-tooth shaped.surfaces (ratchets) are found to accelerate to the right, perpendicular to the vertical thermal gradient. The blue arrows indicate vapour flow which, according to our tentative model, exerts a viscous force on the droplet, pulling it along.

This effect works for all liquids we have cared to try so far (including nitrogen, acetone, methanol, ethanol, water, and hexadecane, with boiling points ranging from - 196 °C to + 151 °C).