Colloidal particles can be irreversibly adsorbed at fluid interfaces, such as oil-water and air-water interfaces. The particle adsorption leads to stabilization of dispersed systems of two immiscible fluids and particle-stabilized (or Pickering) emulsions and foams can be prepared. [1][2][3][4] These materials show some unique properties as a result of adsorption of the particles at the fluid-fluid interface. One of the striking phenomena is that liquid drops can be dispersed in air with the liquid-air surfaces coated by liquid-repellent particles. When the liquid is water, a water-in-air (w/a) material, named dry water, is produced by aerating water in the presence of extremely hydrophobic silica particles. [5][6][7][8][9] The dry water is a free-flowing powder which can contain significant quantities of water as micron-sized drops. One may imagine that when particle-stabilised emulsions with water as the continuous phase, i.e., oilin-water (o/w) emulsions, are aerated with similar hydrophobic particles, the surfaces between the emulsion drops and air can be encased in the hydrophobic particles and oil-in-water-in-air (o/w/a) materials may be prepared, Figure 1a. However, the preparation requires precise tuning of both the properties of the o/w emulsions and the mixing conditions. We have stabilized o/w/a materials using colloidal particles alone and found that control of the coalescence of oil droplets in o/w emulsions on aeration is crucial in the ability to produce powdered emulsions successfully.Dispersed systems consisting of two immiscible fluids, such as emulsions and foams, are usually prepared using molecular or polymeric surfactants. Colloidal particles also act as emulsifiers and foam stabilizers by adsorbing at oil-water and airwater interfaces and forming armoured layers around drops or bubbles, respectively. [1-3] Such particle-stabilized fluid systems show outstanding stability against coalescence and disproportionation. [1,2,10] The driving force for the adsorption of particles to fluid interfaces is the free energy gain in losing an area of interface obliterated by the particles. The types of material formed depend significantly on the wettability of the particles at the interface, quantified by their three-phase contact angle, θ, measured into the water phase. [1,2] It has been shown that, for mixtures of air and water, relatively hydrophilic particles (θ < 90°) preferably form air-in-water (a/w) materials, that is aqueous foams, while relatively hydrophobic particles (θ > 90°) are required for stabilizing water-in-air (w/a) materials. [5][6][7] The w/a materials are represented by water marbles and dry water. The latter behaves like a free-flowing powder but contains a large amount of water (up to 95 wt.% relative to the total mass) as micron-sized droplets. Dry water can be used as a delivery vehicle in the cosmetics and pharmaceutical sectors but also a Ryo Murakami, * Hiroshi Moriyama, Masahiro Yamamoto, Bernard P. Binks,* and Anaïs Rocher Particle Stabilization of Oil-in-Water-in-Air M...