Voltage sensors containing the charged S4 membrane segment display a gating charge vs. voltage (Q-V) curve that depends on the initial voltage. The voltage-dependent phosphatase (Ci-VSP), which does not have a conducting pore, shows the same phenomenon and the Q-V recorded with a depolarized initial voltage is more stable by at least 3RT. The leftward shift of the Q-V curve under prolonged depolarization was studied in the Ci-VSP by using electrophysiological and site-directed fluorescence measurements. The fluorescence shows two components: one that traces the time course of the charge movement between the resting and active states and a slower component that traces the transition between the active state and a more stable state we call the relaxed state. Temperature dependence shows a large negative enthalpic change when going from the active to the relaxed state that is almost compensated by a large negative entropic change. The Q-V curve midpoint measured for pulses that move the sensor between the resting and active states, but not long enough to evolve into the relaxed states, show a periodicity of 120°, indicating a 3 10 secondary structure of the S4 segment when determined under histidine scanning. We hypothesize that the S4 segment moves as a 3 10 helix between the resting and active states and that it converts to an ␣-helix when evolving into the relaxed state, which is most likely to be the state captured in the crystal structures.A number of membrane proteins respond to changes in the membrane electric field via an intrinsic voltage sensor in the protein structure (1). The classical examples, first described by Hodgkin and Huxley (2), are the voltage-dependent sodium and potassium conductances, which are crucial players in the generation and propagation of the nerve impulse. In the voltagegated ion channels that generate these conductances, the movement of the voltage sensor generates a transient current that has been traditionally called gating current, because in the original recordings it was correlated with the opening of the conduction pathway in Na channels (3, 4). Gating currents are transient because the sensing or gating charges are tethered to the protein and so their movement is restricted within the membrane electric field. Most of the moving charges that produce gating currents have been identified as the four most extracellular basic residues of the fourth transmembrane segment (S4) in voltage-gated channels (5, 6).At extremely negative and positive membrane potentials the gating charges are driven to extreme positions so that a plot of the transported charge as a function of the membrane potential (the Q-V curve) has a sigmoid shape that saturates at extreme potentials. The voltage dependence of this charge movement is an expression of the amount of charge involved and the number of states that the sensing charge populates when moving between the extreme positions. The steepness of the Q-V curve in going from one extreme position to the other increases by increasing the moving charge o...