Understanding the structural nature of the free energy bottleneck(s) encountered in protein folding is essential to elucidating the underlying dynamics and mechanism. For this reason, several techniques, including Φ-value analysis, have previously been developed to infer the structural characteristics of such high free-energy or transition states. Herein we propose that one (or few) appropriate...

Most small, single-domain proteins fold with the uncomplicated, single-exponential kinetics expected for diffusion on a smooth energy landscape. Despite this energetic smoothness, the folding rates of these two-state proteins span a remarkable million-fold range. Here, we review the evidence in favor of a simple, mechanistic description, the topomer search model, which quantitatively accounts f...

Recent experimental results suggest that the native fold, or topology, plays a primary role in determining the structure of the transition state ensemble, at least for small fast folding proteins. To investigate the extent of the topological control of the folding process, we study the folding of simplified models of five small globular proteins constructed using a Gō–like potential in order to...

Temperature-sensitive folding mutations (tsf) of the thermostable P22 tailspike protein prevent the mutant polypeptide chain from reaching the native state at the higher end of the temperature range of bacterial growth (37-42 degrees C). At lower temperatures the mutant polypeptide chains fold and associate into native proteins. The melting temperatures of the purified native forms of seven dif...

Elucidating the mechanism of protein folding is an intriguing and challenging task. Currently, tremendous advances have been explored and the combination of experimental and theoretical approaches provides new insights to protein folding [3]. The formation of stable secondary structures and a unique tertiary structure of a protein is mainly dictated by interactions between amino acid residues a...

The rugged folding-energy landscapes of RNAs often display many competing minima. How do RNAs discriminate among competing conformations in their search for the native state? By using optical tweezers, we show that the folding-energy landscape can be manipulated to control the fate of an RNA: individual RNA molecules can be induced into either native or misfolding pathways by modulating the rel...

Experimental studies of protein folding frequently are consistent with two-state folding kinetics. However, recent NMR relaxation dispersion studies of several fast-folding mutants of the Fyn Src homology 3 (SH3) domain have established that folding proceeds through a low-populated on-pathway intermediate, which could not be detected with stopped-flow experiments. The dispersion experiments pro...

The measurement of amino acid-resolved hydrogen exchange (HX) has provided the most detailed information so far available on the structure and properties of protein folding intermediates. Direct HX measurements can define the structure of tenuous molten globule forms that are generally inaccessible to the usual crystallographic and NMR methods (C. Redfield review in this issue). HX pulse labeli...

Recent studies of GroE-mediated protein folding indicate that substrate proteins are productively released from a cis ternary complex in which the nonnative substrate is sequestered within the GroEL channel underneath GroES. Here, we examine whether protein folding can occur in this space. Stopped-flow fluorescence anisotropy of a pyrene-rhodanese-GroEl complex indicates that addition of GroES ...

A simple model of the kinetics of protein folding is presented. The reaction coordinate is the "correctness" of a configuration compared with the native state. The model has a gap in the energy spectrum, a large configurational entropy, a free energy barrier between folded and partially folded states, and a good thermodynamic folding transition. Folding kinetics is described by a master equatio...