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Experimental study of an anti-icing method over an airfoil based on pulsed dielectric barrier discharge plasma 1455 Fig. 9 Anti-icing process of the meshy electrode. Fig. 10 Upper and lower surfaces of the leading edge after the anti-icing process (the meshy electrode case). Fig. 11 Locations of monitoring points for surface temperatures. (3) The specific heat flux needed for the surface water to evaporate (or the specific heat flux needed for ice to sub- lime) (qe). (4) The specific heat flux needed to heat the supercooled droplets collected by the body surface (qw). (5) The specific heat flux converted from the kinetic energy of the water droplets due to their stagnations when col- lected by the body surface (qwv). (6) The specific heat flux radiated from the body surface to the air (qr). (7) The specific heat flux of fusion representing the amount latent heat required to convert unit mass of ice into water without a change in temperature or that released to the surroundings to make unit mass of water freeze (qt).PDF Image | Experimental study of an anti-icing method over an airfoil based on pulsed dielectric barrier discharge plasma
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