An object immersed in a fast flow typically experiences fluid forces that increase with the square of speed. Here we explore how this high-Reynolds-number force-speed relationship is affected by unsteady motions of a body. Experiments on disks that are driven to oscillate while progressing through air reveal two distinct regimes: a conventional quadratic relationship for slow oscillations and an anomalous scaling for fast flapping in which the time-averaged drag increases linearly with flow speed. In the linear regime, flow visualization shows that a pair of counterrotating vortices is shed with each oscillation and a model that views a train of such dipoles as a momentum jet reproduces the linearity. We also show that appropriate scaling variables collapse the experimental data from both regimes and for different oscillatory motions into a single drag-speed relationship. These results could provide insight into the aerodynamic resistance incurred by oscillating wings in flight and they suggest that vibrations can be an effective means to actively control the drag on an object.A central goal of fluid dynamics is to relate the shape and motion of a body to the aerodynamic or hydrodynamic forces it experiences. Investigations into such force laws have formed the basis of fluid physics and engineering and have led to far-reaching applications [1], from minimizing drag by streamlining shapes to generating lift and thus enabling heavier-than-air flight [2]. Studies over the past two centuries have revealed fundamental scaling relationships relating forces to speed for the case of steady flow past a body or, equivalently, steady motion of a body through a fluid. For small objects in slow flows, forces vary in direct proportion to the speed, while large objects in fast flows experience forces that increase as the square of speed [1,3]. These linear and quadratic regimes are demarcated by the Reynolds number, which quantifies the relative importance of fluid inertia to viscosity. Large bodies in fast flows correspond to high Reynolds number and the well-known quadratic drag law stems from the separation of flow from the surface and the associated pressure difference across the body [4].Strongly unsteady motions of a body in a flow are likely to significantly modify flow separation and thus alter force-speed scaling relationships. Such time-dependent motions are common in many contexts. For example, the flow-induced fluttering of flexible structures, such as the flapping of a flag, has recently been studied as an archetype of passively excited oscillations [5][6][7]. Animal locomotion provides examples in which oscillations of structures are actively driven, such as in flying or swimming propelled by flapping wings or fins [8-10]. One feature common to all these problems is the superposition of unsteady or ac motions and steady or dc motions. For the case of locomotion, for example, this involves the oscillations or flapping of an appendage superposed on the body translation during steady forward flight or swimming.Here w...