Acetylcholine-induced flux of inorganic ions across membranes and inactivation of the acetylcholine receptor were measured at pH 7.0, 1@C, over a 5000-fold concentration range of acetylcholine. Receptor-containing electroplax membrane vesicles prepared from Electrophorus electricus and a quench-flow technique were used, allowing flux to be measured in the 2-msec to 1-min time region. Five different measurements were made: (i) rate of ion translocation with the active state of the receptor, (ii) rate of the slower ion translocation after equilibration of active and inactive receptor states, (iii) rate of inactivation, (iv) equilibrium between active and inactive forms of the receptor, and (v) reactivation of inactivated receptor. The kinetics of the steps in the receptor-controlled ion flux follow single-exponential rate laws, and simple analytical expressions for their ligand concentration dependence can be used. Thus, the rate and equilibrium constants in a scheme that relates the ligand binding steps to ion translocation could be evaluated. It was found that the dependence ofthe receptor-controlled ion translocation over the concentration range investigated obeys the integrated rate equation based on the proposed mechanism. The flux rate before inactivation was 107 ions sec-per receptor, which is comparable with that measured electrophysiologically in muscle cells. The half-time ofinactivation is 100 msec when the receptor is saturated with acetylcholine.The specific reaction rate ofthe ion translocation (J) is 3 x 107 M-1 sec '. The results support a minimum reaction mechanism previously proposed on the basis of experiments in which carbamylcholine was used. Nachmansohn (1) first suggested that interaction between acetylcholine and its receptor in nerve and muscle cell membranes induces a conformational change of the protein that results in the formation of ion-conducting channels through the membrane. The consequent translocation of cations results in an electrical signal; the amplitude of which is, determined by the relative rates at which the ions move (2). These rates depend on the number of open receptor-formed channels and, therefore, for a cell containing a given number ofreceptor molecules, on the concentration ofacetylcholine. The amplitude of the signal that determines whether a muscle cell will contract, or whether the signal is propagated ifit is a nerve cell (3), depends therefore on the acetylcholine concentration. This relationship between acetylcholine concentration and receptor-controlled ion flux has been unknown. We have now~made kinetic measurements that allow us to determine the relationship.We have developed methods to measure the rate ofreceptorcontrolled ion flux in the.2-msec to I-min time region (4-11) using membrane vesicles prepared (12) from the electroplax of Electrophorus electricus (13). We chose to use these vesicles rather than Torpedo sp. vesicles because they contain relatively few receptors (about 500 times fewer per unit weight than Torpedo sp. vesicles), and the...