Abstract
Ion pumps perform active transport of ions by using energy. The active transport mechanism can be illustrated by the Panama Canal model, which considers two gates and a gain in energy. The Panama Canal model is consistent with the alternating access model that is used to describe active transport, in which the substrate ion is bound, energized, and released. It was generally accepted that energization occurs only for an ion-bound protein but not for an ion-unbound protein. Light-driven proton and chloride pumps, two of the best studied pumps, are represented by the Panama Canal model. In this case, light absorption takes place for the bound state of ions (proton and chloride ions) in the active center (protonated Schiff base of the retinal chromophore). In contrast, a recently discovered light-driven sodium pump, Krokinobacter eikastus rhodopsin 2 (KR2), is a unique active transporter that does not bind the transport substrate, the sodium ion, in its resting state. The molecular architecture and photoreaction cycle of the light-driven sodium pump are very similar to those of proton and chloride pumps, although sodium ions are actively transported without initial binding. Sodium uptake is a diffusive process, but the presence of two gates allows the unidirectional transport of sodium ions. In this sense, the light-driven sodium pump is also represented by a modified Panama Canal model. Current understanding of the light-driven sodium pump is reviewed.
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