Apparent Debye−Huckel Electrostatic Effects in the Folding of a Simple, Single Domain Protein

Abstract
We have monitored the effects of salts and denaturants on the folding of the simple, two-state protein FynSH3. As predicted by Debye−Huckel limiting law, both the stability and (log) folding rate of FynSH3 increase nearly perfectly linearly (r2 > 0.99) with the square root of ionic strength upon increasing concentrations of the relatively nonchaotropic salt sodium chloride. The stability of FynSH3 is also linear in square root ionic strength when the relatively nonchaotropic salts sodium bromide, potassium bromide, and potassium chloride are employed. Comparison of the kinetic and equilibrium effects of sodium chloride suggests that the electrostatic interactions formed in the folding transition state are approximately 50% as destabilizing as those formed in the native state, presumably reflecting the more compact nature of the latter. In contrast, the relationship between concentration and folding kinetics is more complex when the highly chaotropic salt guanidine hydrochloride (GuHCl) is employed. At moderate to high GuHCl concentrations the net effect of the linear, presumably chaotrope-induced deceleration and the presumed, square root-dependent ionic strength-induced acceleration is well approximated as linear, thus accounting for the observation of “chevron behavior” (log folding rate linear in denaturant concentration) typically reported for the folding of single domain proteins. At very low GuHCl concentrations, however, significant kinetic rollover is observed. This rollover is reasonably well fitted as a sum of a linear, presumably chaotropic effect and a square root-dependent, presumably electrostatic effect. These results thus not only provide insight into the nature of the folding transition state but also suggest that caution is in order when extrapolating GuHCl-based chevrons to estimate folding rates in the absence of denaturant and in interpreting deviations from chevron linearity as evidence for non-two-state kinetics.