The solution structure and dynamics of an Arc repressor mutant reveal premelting conformational changes related to DNA binding.

The solution structure of the hyperstable MYL mutant (R31M/E36Y/R40L) of the Arc repressor of bacteriophage P22 was determined by NMR spectroscopy and compared to that of the wild-type Arc repressor. A backbone rmsd versus the average of 0.37 A was obtained for the well-defined core region. For both Arc-MYL and the wild-type Arc repressor, evidence for a fast equilibrium between a packed ("in") conformation and an extended ("out") conformation of the side chain of Phe 10 was found. In the MYL mutant, the "out" conformation is more highly populated than in the wild-type Arc repressor. The Phe 10 is situated in the DNA-binding beta-sheet of the Arc dimer. While its "in" conformation appears to be the most stable, the "out" conformation is known to be present in the operator-bound form of Arc, where the Phe 10 ring contacts the phosphate backbone [Raumann, B. E., et al. (1994) Nature 367, 754-757]. As well as DNA binding, denaturation by urea and high temperatures induces the functionally active "out" conformation. With a repacking of the hydrophobic core, this characterizes a premelting transition of the Arc repressor. The dynamical properties of the Arc-MYL and the wild-type Arc repressor were further characterized by 15N relaxation and hydrogen-deuterium exchange experiments. The increased main chain mobility at the DNA binding site compared to that of the core of the protein as well as the reorientation of the side chain of Phe 10 is suggested to play an important role in specific DNA binding.

Kinetics and energetics of subunit dissociation/unfolding of TIM: the importance of oligomerization for conformational persistence and chemical stability of proteins.

Kinetics of unfolding and refolding of rabbit muscle triosephosphate isomerase (TIM) were measured as a function of guanidine hydrochloride (GdnHCl) concentration. From the rate constants of these processes, the activation free-energy barriers (delta G++) were calculated using the Arrhenius equation. Assuming a linear dependence of delta G++ on the concentration of GdnHCl, activation energies in the absence of GdnHCl were estimated. The Gibbs free-energy change of dissociation/unfolding (delta G) was determined from GdnHCl unfolding curves in equilibrium. Using these data and the literature value for the bimolecular association rate constant of folded TIM monomers [Zabori, S., Rudolph, R., and Jaenicke, R. (1980) Z. Naturforsch. 35C, 999-1004], a model was developed that fully describes both kinetics and energetics of subunit dissociation/unfolding of TIM. Unfolded TIM monomers are susceptible to proteolytic digestion and thiol oxidation, while native TIM is resistant to both. The present model explains how the dimeric nature of TIM decreases the frequency of subunit unfolding by several orders of magnitude, thus increasing the chemical stability of the protein. Furthermore, the model also explains the recently demonstrated persistence (on a time scale of hours to days) of conformational heterogeneity of native TIM dimers [Rietveld, A. W. M., and Ferreira, S. T. (1996) Biochemistry 35, 7743-7751]. Again, it appears that the dimeric nature of TIM is essential for this behavior.

Deterministic pressure dissociation and unfolding of triose phosphate isomerase: persistent heterogeneity of a protein dimer.

Subunit dissociation and unfolding of dimeric rabbit muscle triose phosphate isomerase (TIM) induced by hydrostatic pressure were investigated. Changes in fluorescence emission of TIM (both intrinsic and of covalently attached probes) indicated that pressure ranging from 1 bar to 3.5 kbar promoted subunit dissociation and unfolding. Instrinsic fluorescence changes upon unfolding by pressure included a 27 nm red-shift of the emission, a decrease in fluorescence anisotropy from 0.14 to about 0.01, and a 1.5-fold increase in fluorescence quantum yield, similar to that observed in the presence of guanidine hydrochloride. Kinetics of pressure-induced fluorescence changes were slow (t 1/2 approximately 15 min) and little dependent on pressure. In order to selectively monitor subunit dissociation, fluorescence resonance energy transfer (FRET) measurements were carried out with TIM that was separately labeled with 5-((((2-iodoacetyl)-amino)ethyl)amino)naphthalene-1-sulfonic acid (1,5-IAEDANS) or fluorescein-5-isothiocyanate (FITC). FRET measurements indicated that subunit dissociation and unfolding took place concomitantly, both under equilibrium conditions and in kinetic experiments in which dissociation/unfolding was triggered by a sudden increase in pressure. Release of pressure caused monomer refolding and dimerization. Contrary to what would be expected for a process involving subunit dissociation, pressure effects on TIM were not dependent on protein concentration. Experiments involving a series of pressure jumps demonstrated persistent heterogeneity in sensitivity toward pressure in the ensemble of TIM dimers. This kind of deterministic behavior is similar to that exhibited by higher order protein aggregates and indicates that not all individual dimers are energetically identical in solution. The heterogeneity of native TIM revealed by sensitivity to pressure could not be detected by traditional means of protein separation, such as polyacrylamide gel electrophoresis (under both native and denaturing conditions) and size exclusion gel chromatography. This suggests that energetic heterogeneity originates from conformational heterogeneity of the protein. The possible biological relevance of the deterministic character of stability of TIM is discussed.

Effect of hydrostatic pressure on the fluorescence of indole derivatives.

Effects of hydrostatic pressure on the fluorescence emission of L-tryptophan, N-acetyl-L-trytophanamide and indole were investigated. An increase in pressure ranging from 1 bar to 2.4 kbar results in reversible red-shifts of the emission of the three fluorophores. The pressure-induced redshift amounts to about 170 cm(-1) at 2.4 kbar, and appears related to changes in Stokes shift of the fluorophores caused by pressure effects on the dielectric constant and/or refractive index of the medium. As the pressure range investigated here is the range commonly used in studies of protein subunit association and/or folding, these observations raise the need for caution in interpreting pressure-induced spectral shifts. The significance of these observations to pressure studies of proteins is illustrated by investigation of pressure effects on human Cu,Zn Superoxide dismutase (SOD) and azurin fromPseudomonas aeruginosa. A reversible 170 cm(-1) red-shift of the emission of SOD was observed upon pressurization to 2.4 kbar. This might be interpreted as pressure-induced conformational changes of the protein. However, further studies using SOD that had been fully unfolded by guanidine hydrochloride, and fluorescence anisotropy measurements indicated that the observed red-shift was likely due to a direct effect of pressure on the fluorescence of the single tryptophan residue of SOD. Similar pressure-induced red-shifts were also observed for the buried tryptophan residue of azurin or for azurin that had been previously denatured by guanidine hydrochloride. These observations further suggest that the effective dielectric constant of the protein matrix is affected by pressure similarly to water.