(A1) When channels that are permeable for a single ion species only are activated (depicted as conductance, G), the current that is needed to charge the membrane capacitance Cm to the equilibrium potential of this ion (E) is negligible. Hence, the net ion flux across the membrane is very small. (A2) During coactive excitation and inhibition, glutamate-and GABA-gated ion channels (GNa and GCl, respectively) are activated. A simultaneous influx of the oppositely charged Na+ and Cl− ions, driven by the ionic electrochemical gradients (Vm−ENa and Vm−ECl), takes place. Therefore, most of the net influx of the Na+ and Cl− ions is electrically neutral (see ).
(B) Simplified scheme depicting channel and transporter mediated ionic fluxes at excitatory and inhibitory synapses, where the net influx of Cl− and Na+ ions across glutamate- and GABA-gated ion channels is counteracted by the K-Cl cotransporter KCC2 (or some other KCC isoform) and by the Na-K ATPase. K+ accumulation by the Na-K AT-Pase leads typically to values of EK of about −100 mV, which is a fundamental requirement for hyperpolarizing GABAergic inhibition: the K+ electrochemical gradient sets the driving force for Cl− extrusion by KCC2. Because the Na-K ATPase takes up two K+ ions for one cycle of ATP hydrolysis, two Cl− ions are extruded at the expense of one ATP. Hence, one cycle of the Na-K pump that consumes one ATP molecule can offset the influx of two Cl− ions and three Na+ ions. “Out” and “in” refer to the extracellular and intracellular compartments, respectively. In (A2), the Hodgkin-Huxley convention of setting the polarities of ENa and ECl was adopted.