Mechanical unfolding of spectrin reveals a super-exponential dependence of unfolding rate on force.

We investigated the mechanical unfolding of single spectrin molecules over a broad range of loading rates and thus unfolding forces by combining magnetic tweezers with atomic force microscopy. We find that the mean unfolding force increases logarithmically with loading rate at low loading rates, but the increase slows at loading rates above 1pN/s. This behavior indicates an unfolding rate that increases exponentially with the applied force at low forces, as expected on the basis of one-dimensional models of protein unfolding. At higher forces, however, the increase of the unfolding rate with the force becomes faster than exponential, which may indicate anti-Hammond behavior where the structures of the folded and transition states become more different as their free energies become more similar. Such behavior is rarely observed and can be explained by either a change in the unfolding pathway or as a reflection of a multidimensional energy landscape of proteins under force.

ATP-dependent proteases degrade their substrates by processively unraveling them from the degradation signal.

Protein unfolding is a key step in several cellular processes, including protein translocation across some membranes and protein degradation by ATP-dependent proteases. ClpAP protease and the proteasome can actively unfold proteins in a process that hydrolyzes ATP. Here we show that these proteases seem to catalyze unfolding by processively unraveling their substrates from the attachment point of the degradation signal. As a consequence, the ability of a protein to be degraded depends on its structure as well as its stability. In multidomain proteins, independently stable domains are unfolded sequentially. We show that these results can explain the limited degradation by the proteasome that occurs in the processing of the precursor of the transcription factor NF-kappaB.

Effect of the protein import machinery at the mitochondrial surface on precursor stability.

Many biological processes require proteins to undergo conformational changes at the surface of membranes. For example, some precursor proteins unfold at the surface of mitochondria and chloroplasts before translocation into the organelles, and toxins such as colicin A unfold to the molten globule state at bacterial surfaces before inserting into the cell membrane. It is commonly thought that the membrane surfaces and the associated protein machinery destabilize the substrate proteins and that this effect is required for membrane insertion or translocation. One of the best characterized translocation processes is protein import into mitochondria. By measuring the contributions of individual interactions within a model protein to its stability at the mitochondrial surface and in free solution, we show here that the mitochondrial surface neither induces the molten globule state in this protein nor preferentially destabilizes any type of interaction (e.g., hydrogen bonds, nonpolar, etc.) within the protein. Because it is not possible to measure absolute protein stability at the surface of mitochondria, we determined the stability of a tightly associated protein-protein complex at the mitochondrial import site as a model of the stability of a protein. We found the binding constants of the protein-protein complex at the mitochondrial surface and in free solution to be identical. Our results demonstrate that the mitochondrial surface does not destabilize importing precursor proteins in its vicinity.

Protein unfolding by mitochondria. The Hsp70 import motor.

Protein unfolding is a key step in the import of some proteins into mitochondria and chloroplasts and in the degradation of regulatory proteins by ATP-dependent proteases. In contrast to protein folding, the reverse process has remained largely uninvestigated until now. This review discusses recent discoveries on the mechanism of protein unfolding during translocation into mitochondria. The mitochondria can actively unfold preproteins by unraveling them from the N-terminus. The central component of the mitochondrial import motor, the matrix heat shock protein 70, functions by both pulling and holding the preproteins.

Mitochondria unfold precursor proteins by unraveling them from their N-termini.

Protein unfolding is a key step in the life cycle of many proteins, including certain proteins that are degraded by ATP-dependent proteases or translocated across membranes. The detailed mechanisms of these unfolding processes are not understood. Precursor proteins are unfolded and imported into mitochondria by a macromolecular machine that spans two membranes and contains at least nine different proteins. Here we examine import of a model precursor protein derived from the ribonuclease barnase and show that mitochondria unfold this protein by unraveling it from its N-terminus. Because barnase in free-solution unfolds by a different pathway, our results demonstrate that mitochondria catalyze unfolding in the way that enzymes catalyze reactions, namely by changing reaction pathways. The effectiveness of this mechanism depends on the structure of the N-terminal part of the precursor protein.

The dimensions of the protein import channels in the outer and inner mitochondrial membranes.

Most mitochondrial proteins are imported into mitochondria through transmembrane channels composed largely, and perhaps exclusively, of proteins. We have determined the effective internal diameter of the protein import channel in the mitochondrial outer membrane to be between 20 A and 26 A during translocation. The diameter of the import channel in the inner membrane is smaller than the diameter of the outer membrane import channel. These results were obtained by measuring the effect of rigid steric bulk introduced into precursor proteins on import.

The structure of precursor proteins during import into mitochondria.

Precursor proteins must be at least partially unfolded during import into mitochondria, but their actual conformation during translocation is not known. Are proteins fully unfolded and threaded through the import machinery amino acid by amino acid, or do they retain some partial structure? The folding pathway of most proteins in vitro contains a partially folded intermediate known as the molten globule state, and it has been suggested that proteins are in the molten globule state during translocation across membranes. Here we show that precursors are normally fully unfolded during import into mitochondria. However, precursors containing residual structure can be imported, if less efficiently.

Active unfolding of precursor proteins during mitochondrial protein import.

Precursor proteins made in the cytoplasm must be in an unfolded conformation during import into mitochondria. Some precursor proteins have tightly folded domains but are imported faster than they unfold spontaneously, implying that mitochondria can unfold proteins. We measured the import rates of artificial precursors containing presequences of varying length fused to either mouse dihydrofolate reductase or bacterial barnase, and found that unfolding of a precursor at the mitochondrial surface is dramatically accelerated when its presequence is long enough to span both membranes and to interact with mhsp70 in the mitochondrial matrix. If the presequence is too short, import is slow but can be strongly accelerated by urea-induced unfolding, suggesting that import of these 'short' precursors is limited by spontaneous unfolding at the mitochondrial surface. With precursors that have sufficiently long presequences, unfolding by the inner membrane import machinery can be orders of magnitude faster than spontaneous unfolding, suggesting that mhsp70 can act as an ATP-driven force-generating motor during protein import.

Hsp60-independent protein folding in the matrix of yeast mitochondria.

Proteins that are imported from the cytosol into mitochondria cross the mitochondrial membranes in an unfolded conformation and then fold in the matrix. Some of these proteins require the chaperonin hsp60 for folding. To test whether hsp60 is required for the folding of all imported matrix proteins, we monitored the folding of four monomeric proteins after import into mitochondria from wild-type yeast or from a mutant strain in which hsp60 had been inactivated. The four precursors included two authentic matrix proteins (rhodanese and the mitochondrial cyclophilin Cpr3p) and two artificial precursors (matrix-targeted variants of dihydrofolate reductase and barnase). Only rhodanese formed a tight complex with hsp60 and required hsp60 for folding. The three other proteins folded efficiently without, and showed no detectable binding to, hsp60. Thus, the mitochondrial chaperonin system is not essential for the folding of all matrix proteins. These data agree well with earlier in vitro studies, which had demonstrated that only a subset of proteins require chaperones for efficient folding.

Movement of the position of the transition state in protein folding.

Hammond behavior, in which two neighboring states move closer to each other along the reaction coordinate as the energy difference between them becomes smaller, has previously been observed for the transition state of unfolding of barnase. Here, we report Hammond behavior for the small protein chymotrypsin inhibitor 2 (CI2), which folds and unfolds via a single rate-determining transition state and simple two-state kinetics. Mutants have been generated along the entire sequence of the protein and the kinetics of folding and unfolding measured as a function of concentration of denaturant. The transition state was found to move progressively closer to the folded state on destabilization of the protein by mutation. Different regions of CI2 all show a similar sensitivity to changes in the energy of the transition state. This is in contrast to the behavior of barnase on mutation for which the position of the transition state for its unfolding is sensitive to mutation in some regions, especially in its major alpha-helix, but not in others. The transition state for the folding and unfolding of CI2 resembles an expanded version of the folded state and is formed in a concerted manner, in contrast to that for barnase, in which some regions of structure are fully formed and others fully unfolded. The reason for the general sensitivity of the position of the transition state of CI2 to mutation is presumably the relatively uniform degree of structure formation in the transition state and the concerted nature of its formation.(ABSTRACT TRUNCATED AT 250 WORDS)

Cyclophilin catalyzes protein folding in yeast mitochondria.

Cyclophilins are a family of ubiquitous proteins that are the intracellular target of the immunosuppressant drug cyclosporin A. Although cyclophilins catalyze peptidylprolyl cis-trans isomerization in vitro, it has remained open whether they also perform this function in vivo. Here we show that Cpr3p, a cyclophilin in the matrix of yeast mitochondria, accelerates the refolding of a fusion protein that was synthesized in a reticulocyte lysate and imported into the matrix of isolated yeast mitochondria. The fusion protein consisted of the matrix-targeting sequence of subunit 9 of F1F0-ATPase fused to mouse dihydrofolate reductase. Refolding of the dihydrofolate reductase moiety in the matrix was monitored by acquisition of resistance to proteinase K. The rate of refolding was reduced by a factor of 2-6 by 2.5 microM cyclosporin A. This reduced rate of folding was also observed with mitochondria lacking Cpr3p. In these mitochondria, protein folding was insensitive to cyclosporin A. The rate of protein import was not affected by cyclosporin A or by deletion of Cpr3p.

Extrapolation to water of kinetic and equilibrium data for the unfolding of barnase in urea solutions.

Assumptions about the dependence of protein unfolding on the concentration of urea have been examined by an extensive survey of the equilibrium unfolding of barnase and many of its mutants measured by urea denaturation and differential scanning calorimetry. The free energy of equilibrium unfolding and the activation energy for the kinetics of unfolding of proteins are generally assumed to change linearly with [urea]. A slight downward curvature is detected, however, in plots of highly precise measurements of logku versus [urea] (where ku is the observed rate constant for the unfolding of barnase). The data fit the equation logku = logkuH2O* + mku*.[urea] - 0.014[urea]2, where mku* is a variable which depends on the mutation. The constant 0.014 was measured directly on four destabilized mutants and wild-type, and was also determined from a global analysis of data from > 60 mutants of barnase. Any equivalent deviations from linearity in the equilibrium unfolding are small and in the same region, as determined from measurements on 166 mutants. The free energy of unfolding of barnase, delta GU-F, appears significantly larger by 1.6 kcal mol-1 when measured by calorimetry than when determined by urea denaturation. However, the changes in delta GU-F on mutation, delta delta GU-F, determined by calorimetry and by urea denaturation are identical. We show analytically how, in general, the curvature in plots of activation or equilibrium energies against [denaturant] should not affect the changes of these values on mutation provided measurements are made over the same concentration ranges of denaturant and the curvature is independent of mutation.

Application of physical organic chemistry to engineered mutants of proteins: Hammond postulate behavior in the transition state of protein folding.

Transition states in protein folding may be analyzed by linear free-energy relationships (LFERs) analogous to the Brønsted equation for changes in reactivity with changes in structure. There is an additional source of LFERs in protein folding: the perturbation of the equilibrium and rate constants by denaturants. These LFERs give a measure of the position of the transition state along the reaction coordinate. The transition state for folding/unfolding of barnase has been analyzed by both types of LFERs: changing the structure by protein engineering and perturbation by denaturants. The combination has allowed the direct monitoring of Hammond postulate behavior of the transition state on the reaction pathway. Movement of the transition state has been found and analyzed to give further details of the order of events in protein folding.

The folding of an enzyme. I. Theory of protein engineering analysis of stability and pathway of protein folding.

The theory, assumptions and limitations are outlined for a simple protein engineering approach to the problem of the stability and pathway of protein folding. It is a general procedure for analysing structure-activity relationships in non-covalent bonding, including enzyme catalysis, that relates experimentally accessible data to changes in non-covalent bonding. Kinetic and equilibrium measurements on the unfolding and refolding of mutant proteins can be used to map the formation of structure in transition states and folding intermediates. For example, the ratio of the changes in the activation energy of unfolding and the free energy of unfolding on mutation is measured to give a parameter phi. There are two extreme values of phi that are often found in practice and may be interpreted in a simple manner. A value of phi = 0 implies that the structure at the site of mutation is as folded in the transition state as it is in the folded state. Conversely, phi = 1 shows that the structure at the site of mutation is as unfolded in the transition state as it is in the unfolded structure. Fractional values of phi are more difficult to interpret and require a more sophisticated approach. The most suitable mutations involve truncation of side-chains to remove moieties that preferably make few interactions with the rest of the protein and do not pair with buried charges. Fractional values of phi found for this type of mutation may imply that there is partial non-covalent bond formation or a mixture of states. The major assumptions of the method are: (1) mutation does not alter the pathway of folding; (2) mutation does not significantly change the structure of the folded state; (3) mutation does not perturb the structure of the unfolded state; and (4) the target groups do not make new interactions with new partners during the course of reaction energy. Assumptions (2) and (3) are not necessarily essential for the simple cases of phi = 0 or 1, the most common values, since effects of disruption of structure can cancel out. Assumption (4) may be checked by the double-mutant cycle procedure, which may be analysed to isolate the effects of just a pair of interactions against a complicated background. This analysis provides the formal basis of the accompanying studies on the stability and pathway of folding of barnase, where it is seen that the theory holds very well in practice.

The folding of an enzyme. II. Substructure of barnase and the contribution of different interactions to protein stability.

Barnase is described anatomically in terms of its substructures and their mode of packing. The surface area of hydrophobic residues buried on formation and packing of the structural elements has been calculated. Changes in stability have been measured for 64 mutations, 41 constructed in this study, strategically located over the protein. The purpose is to provide: (1) information on the magnitudes of changes in stabilization energy for mutations of residues that are important in maintaining the structure; and (2) probes for the folding pathway to be used in subsequent studies. The majority of mutations delete functional moieties of side-chains or make isosteric changes. The energetics of the interactions are variable and context-dependent. The following general conclusions may be drawn, however, from this study about the classes of interactions that stabilize the protein. (1) Truncation of buried hydrophobic side-chains has, in general, the greatest effect on stability. For fully buried residues, this averages at 1.5 kcal mol-1 per methylene group with a standard deviation of +/- 0.6 kcal mol-1. Truncation of partly exposed leucine, isoleucine or valine residues that are in the range of 50 to 80 A2 of solvent-accessible area (30 to 50% of the total solvent-accessible area on a Gly-X-Gly tripeptide, i.e. those packed against the surface) has a smaller, but relatively constant effect on stability, at 0.81 kcal mol-1 per methylene group with a statistical standard deviation of +/- 0.18 kcal mol-1. (2) There is a very poor correlation between hydrophobic surface area buried and the free energy change for an extensive data set of hydrophobic mutants. The best correlation is found to be between the free energy change and the number of methylene groups within a 6 A radius of the hydrophobic groups deleted. (3) Burial of the hydroxyl group of threonine in a pocket that is intended for a gamma-methyl group of valine costs 2.5 kcal mol-1, in the range expected for the loss of two hydrogen bonds.(ABSTRACT TRUNCATED AT 400 WORDS)

The folding of an enzyme. III. Structure of the transition state for unfolding of barnase analysed by a protein engineering procedure.

The structure of the first significant transition state on the unfolding pathway of barnase has been analysed in detail by protein engineering methods. Over 50 mutations placed strategically over the whole protein have been used as probes to report on the local structure in the transition state. Several different probes for many regions of the protein give consistent results as do multiple probes at the same site. The overall consistency of phi values indicates that the mutations have not produced changes in the protein that significantly alter the transition state for unfolding. A fine-structure analysis of interactions has also been conducted by removing different parts of the same side-chains. Many of the results of simple mutations fall nicely into the two clear-cut cases of phi = 1 or 0, indicating that the local noncovalent bonds are either fully broken or fully made in the transition state. Much of the structure of barnase in the transition state for unfolding is very similar to that in the folded protein. Both major alpha-helices fray at the N terminus. The last two turns in helix1 are certainly intact, as is the C terminus of helix2. The general picture of the beta-sheet is that the three central beta-strands are completely intact while the two edge beta-strands are mainly present but certainly weakened. The first five residues of the protein unwind but the C terminus remains folded. Three of the five loops are unfolded. The edges of the main hydrophobic core (core1) are significantly weakened, however, and their breaking appears partly rate determining. The centre of the small hydrophobic core3 remains intact. Core2 is completely disrupted. The first events in unfolding are thus: the unfolding of several loops, the unwinding of the helices from the N termini, and the weakening and disruption of the hydrophobic cores. The values of phi are found to be substantially the same under conditions that favour folding as under conditions that are highly denaturing, and so the structure of the unfolding transition state is substantially the same in water as in the presence of denaturant. The structure of the final kinetically significant transition state for refolding is identical to that for unfolding. The final events in refolding are, accordingly, the consolidation of the hydrophobic cores, the closing of many loops and the capping of the N termini of the helices.

The folding of an enzyme. IV. Structure of an intermediate in the refolding of barnase analysed by a protein engineering procedure.

The pathway of refolding of barnase has been analysed by the protein engineering method using phi plots. The description comprises a folding intermediate, a major transition state (the unfolding transition state) and the fully folded structure. Over 40 mutations have been analysed in the different structural motifs, frequently with several probes in each region. Many of the mutations in this study give phi values for formation of the intermediate of 0, showing that the relevant regions of the structure are as fully unfolded in the intermediate as the unfolded state. Some folding phi values are close to unity, indicating that those regions are fully formed in the intermediate. Even if the data do not report back on a single intermediate but give the averaged properties of a heterogeneous population of sequential or parallel intermediates, then this simplicity of phi data shows that the intermediates tend to have structural features in common. Many phi values are intermediate between those for the unfolded state and the transition state, consistent with either partial structure formation in a single intermediate or a heterogeneous mixture of populations, although the former is more likely. The data are consistent with the intermediate, or collection of intermediates, being on the reaction pathway, rather than side products, because the phi values increase throughout the folding pathway. The main conclusions on the formation of substructure and sequence of folding events from the phi plots are as follows. (1) The major hydrophobic core (core1) begins to form in the intermediate and strengthens in the major transition state. The centre of the core is formed earlier and is stronger in the intermediate and in the transition state than are the edges. (2) Core2 is not formed until after the major transition state. (3) Core3 begins to form in the intermediate and is compact in the transition state. (4) Loop2, loop4 and part of loop1 do not fold until after the major transition state, but the guanosine-binding loop (loop3) is formed in the intermediate and loop5 is partially formed in the intermediate and the transition state. (5) The centre of the beta-sheet is substantially formed in the intermediate, and is fully present in the transition state, but the edges, and associated turns, are definitely weakened.(ABSTRACT TRUNCATED AT 400 WORDS)