We studied the detachment of sessile droplets of conductive liquids from an immersed wire by reducing the contact angle using ac electrowetting. Upon detachment, the droplets acquire a certain amount of charge, which is shown to be controlled by a dimensionless parameter . describes the interplay between the diverging Ohmic resistance of the breaking capillary neck and the ac frequency. In the specific configuration of the present experiment, discharging at high frequency leads to self-excited oscillations in which the droplets periodically detach from and reattach to the wire. DOI: 10.1103/PhysRevLett.96.016106 PACS numbers: 68.03.ÿg, 68.05.ÿn, 83.60.Np The manipulation of tiny amounts of liquids has become a paradigm in various fields of applied physics such as printing and coating technology or biotechnology related microfluidics. Pressure gradients for driving fluid motion are traditionally generated using mechanical, thermomechanical, or electrical actuators. Given the intrinsically high surface to volume ratio in microfluidics, on-demand variations of interfacial energies such as thermocapillary effects [1] and electrowetting [2] have received increasing attention in recent years. The interplay of surface tension and electric fields can also be used to generate liquid jets [3] and droplets, for example in electrospray ionization [4,5] or in continuous ink-jet printing [6]. The role of the electric field in these examples is twofold: on the one hand, it drives the instability leading to the generation and detachment of microdroplets from the reservoir. On the other hand, it is responsible for the charge acquired by the detached droplets. In common configurations using dc voltage both aspects are tightly coupled. In the present Letter, we use low frequency ac electrowetting to detach liquid droplets from an electrode. We will show that the amount of charge acquired by a droplet detaching can be controlled by tuning the electrical properties of the liquid and the applied ac frequency. In this process, the breakup of the capillary neck in the late stage of the detachment process plays a crucial role. In conjunction with the finite conductivity of typical aqueous liquids, the algebraic decrease of the neck diameter [7,8] gives rise to a continuous divergence of the neck's Ohmic resistance. The speed of this divergence compared to the ac frequency determines to what extent the detaching droplet can be discharged.Droplets of a conductive liquid (volume 1 l, various mixtures of deionized water, glycerol, and NaCl) were deposited on conductive substrates that are covered by a thin insulating layer and a hydrophobic top coating (1 m thick thermally grown SiO 2 covered by a hydrophobic selfassembled monolayer of Octadecyltrichlorosilane [9]). The composition of the liquid was varied to cover a range of viscosities and conductivities from 2 mPa s to 70 mPa s and from 0.1 to 10 mS=cm, respectively. The entire system was immersed in a silicone oil bath (Fluka, viscosity 5 mPa s) in order to reduce both contact angle...