The last phase of the proton transfer cycle of bacteriorhodopsin calls for a passage of a proton from D38 to D96.This reaction utilizes a narrow shaft ;10-A˚ long that connects the two carboxylates that cross through a very hydrophobicdomain. As the shaft is too narrow to be permanently hydrated, there are two alternatives for the proton propagation into thechannel. The proton may propagate through the shaft without solvation at the expense of a high electrostatic barrier;alternatively, the shaft will expand to accommodate some water molecules, thus lowering the Born energy for the insertion ofthe charge into the protein (B. Scha¨ tzler, N. A. Dencher, J. Tittor, D. Oesterhelt, S. Yaniv-Checover, E. Nachliel, and G. Gutman,2003, Biophys. J. 84:671–686). A comparative study of nine published crystal-structures of bacteriorhodopsin identified, next tothe shaft, microcavities in the protein whose position and surrounding atoms are common to the reported structures. Some ofthe cavities either shrink or expand during the photocycle. It is argued that the plasticity of the cavities provides a working spaceneeded for the transient solvation of the shaft, thus reducing the activation energy necessary for the solvation of the shaft. Thissuggestion is corroborated by the recent observations of Klink et al. (B. U. Klink, R. Winter, M. Engelhard, and I. Chizhov, 2002,Biophys. J. 83:3490–3498) that the late phases of the photocycle (t $ 1 ms) are strongly inhibited by external pressure.