We investigate theoretically and experimentally the capillary-gravity waves created by a small object moving steadily at the water-air interface along a circular trajectory. It is well established that, for straight uniform motion, no steady waves appear at velocities below the minimum phase velocity cmin = 23 cm · s −1 . We show theoretically that no such velocity threshold exists for a steady circular motion, for which, even for small velocities, a finite wave drag is experienced by the object. This wave drag originates from the emission of a spiral-like wave pattern. Our results are in good agreement with direct experimental observations of the wave pattern created by a circularly moving needle in contact with water. Our study leads to new insights into the problem of animal locomotion at the water-air interface.PACS numbers: 47.35.-i , 68.03.-g Capillary-gravity waves propagating at the free surface of a liquid are driven by a balance between the liquid inertia and its tendency, under the action of gravity and surface tension forces, to return to a state of stable equilibrium [1]. For an inviscid liquid of infinite depth, the dispersion relation relating the angular frequency ω to the wave number k is given by ω 2 = gk + γk 3 /ρ, where ρ is the liquid density, γ the liquid-air surface tension, and g the acceleration due to gravity [2]. The above equation may also be written as a dependence of the wave velocity c(k) = ω(k)/k on wave number: c(k) = (g/k + γk/ρ) 1/2 . The dispersive nature of capillary-gravity waves is responsible for the complicated wave pattern generated at the free surface of a still liquid by a moving disturbance such as a partially immersed object (e.g. a boat or an insect) or an external surface pressure source [2,3,4,5,6]. Since the disturbance expends a power to generate these waves, it will experience a drag, R w , called the wave resistance [3]. In the case of boats and large ships, this drag is known to be a major source of resistance and important efforts have been devoted to the design of hulls minimizing it [7]. The case of objects small relative to the capillary length κ −1 = (γ/(ρg)) 1/2 has only recently been considered [8,9,10,11].In the case of a disturbance moving at constant velocity V , the wave resistance R w cancels out for V < c min where V stands for the magnitude of the velocity, and c min = (4gγ/ρ) 1/4 is the minimum of the wave velocity c(k) given above for capillarity gravity waves [3,4,8]. For water with γ = 73 mN · m −1 and ρ = 10 3 kg · m −3 , one has c min = 0.23 m · s −1 (room temperature). This striking behavior of R w around c min is similar to the well-known Cerenkov radiation emitted by a charged particle [12], and has been recently studied experimentally [13,14]. In this letter, we demonstrate that just like accelerated charged particles radiate electromagnetic waves even while moving slower than the speed of light [15], an accelerated disturbance experiences a non-zero wave resistance R w even when propagating below c min . We consider the special cas...