In a previous paper, on “Heat Transfer between Metal Pipes and a Stream of Air”, presented to the Institution in 1933, an account was given of measurements on the transfer of heat between plain pipes and a stream of air. The present paper is an extension of this investigation to gilled pipes. Observations have been made on the heat loss from four gilled pipes of diameters between 1 and 2½ inches, with gills varying in diameter from 2 to 4⅓ inches. Each pipe was studied as a single unit in the wind tunnel, whilst one size of pipe was also examined when built into a battery of similar pipes placed with their axes across the direction of the air flow. The result found for plain pipes, namely, that H/ κ θ is a function of V d/ v only (where H is the heat loss per unit length from a pipe of diameter d at a temperature excess θ over air of thermal conductivity κ and kinematic viscosity v, moving at velocity V), requires modification in the case of gilled pipes. In the former case, H is the heat loss per unit length, and is thus equivalent to the product of the circumference and the heat loss per unit area. The latter interpretation, when dealing with the results for the gilled pipes, does not give systematic results, if the heat loss per unit area is calculated on the total exposed area of the pipe. Moreover, in defining the surface emitting heat, the quantity d, the pipe diameter, is only unambiguous for plain pipes. In the case of gilled pipes, it is found that the most consistent treatment of the results is obtained if d is taken to be the “effective diameter” of the pipe, i.e. the total exposed area per unit length divided by π If the interpretations just explained are given to the quantities H and d, then it is found that to a first approximation, the relationship between H/ κ θ and V d/ v is the same for a gilled and a plain pipe. The observations have also been analysed from the point of view of the temperature of the edge of the gill, relative to that of the air and that of the pipe.