Toward the realization of nanoscale device control, we report a molecular valve embedded in a membrane that can be opened by illumination with long-wavelength ultraviolet (366 nanometers) light and then resealed by visible irradiation. The valve consists of a channel protein, the mechanosensitive channel of large conductance (MscL) from Escherichia coli, modified by attachment of synthetic compounds that undergo light-induced charge separation to reversibly open and close a 3-nanometer pore. The system is compatible with a classical encapsulation system, the liposome, and external photochemical control over transport through the channel is achieved.

The selectivity filter of the bacterial porin OmpF carries a small net charge close to -1 e and is therefore only slightly cation-selective. Calcium channels, on the other hand, contain four negatively charged glutamates, the EEEE-locus, and are among the most selective cation channels known. We aimed to turn the essentially nonselective OmpF into a Ca2+-selective channel. To that end, two additional glutamates (R42E and R132E) were introduced in the OmpF constriction zone that already contains D113 and E117. Mutant OmpF containing this DEEE-locus has a high Ca2+ over Cl- selectivity and a Na+ current with a strongly increased sensitivity to 1 mM Ca2+. The charge/space competition model, initially applied to the L-type Ca2+ channel, identifies the fixed charge and filter volume as key determinants of ion selectivity, with the precise atomic arrangement having only second-order effects. By implication, the reproduction of fixed charge and filter volume should transform two channels into channels of similar selectivity, even if the two belong to entirely different ion channel families, as is the case for OmpF and the L-type Ca2+ channel. The results presented here fit quite well in the framework of charge/space competition theory.

The folding of an 85-residue protein, the histidine-containing phosphocarrier protein HPr, has been studied using a variety of techniques including DSC, CD, ANS fluorescence, and NMR spectroscopy. In both kinetic and equilibrium experiments the unfolding of HPr can be adequately described as a two-state process which does not involve the accumulation of intermediates. Thermodynamic characterization of the native and the transition states has been achieved from both equilibrium and kinetic experiments. The heat capacity change from the denatured state to the transition state (3. 2 kJ mol-1 K-1) is half of the heat capacity difference between the native and denatured states (6.3 kJ mol-1 K-1), while the solvent accessibility of the transition state (0.36) indicates that its compactness is closer to that of the native than that of the denatured state. The high value for the change in heat capacity upon unfolding results in the observation of cold denaturation at moderate denaturant concentrations. Refolding from high denaturant concentrations is, however, slow. The rate constant of folding in water, (14.9 s-1), is small compared to that reported for other proteins of similar size under similar conditions. This indicates that very fast refolding is not a universal character of small globular proteins which fold in the absence of detectable intermediates.

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