A Two-step Mechanism for the Folding of Actin by the Yeast Cytosolic Chaperonin

Actin requires the chaperonin containing TCP1 (CCT), a hexadecameric ATPase essential for cell viability in eukaryotes, to fold to its native state. Following binding of unfolded actin to CCT, the cavity of the chaperone closes and actin is folded and released in an ATP-dependent folding cycle. In yeast, CCT forms a ternary complex with the phosducin-like protein PLP2p to fold actin, and together they can return nascent or chemically denatured actin to its native state in a pure in vitro folding assay. The complexity of the CCT-actin system makes the study of the actin folding mechanism technically challenging. We have established a novel spectroscopic assay through selectively labeling the C terminus of yeast actin with acrylodan and observe significant changes in the acrylodan fluorescence emission spectrum as actin is chemically unfolded and then refolded by the chaperonin. The variation in the polarity of the environment surrounding the fluorescent probe during the unfolding/folding processes has allowed us to monitor actin as it folds on CCT. The rate of actin folding at a range of temperatures and ATP concentrations has been determined for both wild type CCT and a mutant CCT, CCT4anc2, defective in folding actin in vivo. Binding of the non-hydrolysable ATP analog adenosine 5′-(β,γ-imino)triphosphate to the ternary complex leads to 3-fold faster release of actin from CCT following addition of ATP, suggesting a two-step folding process with a conformational change occurring upon closure of the cavity and a subsequent final folding step involving packing of the C terminus to the native-like state.     

Thermal unfolding of G-actin monitored with the DNase I-inhibition assay stabilities of actin isoforms.

Actin is one of the proteins that rely on chaperonins for proper folding. This paper shows that the thermal unfolding of G-actin, as studied by CD and ultraviolet difference spectrometry, coincides with a loss in DNase I-inhibiting activity of the protein. Thus, the DNase I inhibition assay should be useful for systematic studies of actin unfolding and refolding. Using this assay, we have investigated how the thermal stability of actin is affected by either Ca2 + or Mg2 + at the high affinity divalent cation binding site, by the concentration of excess nucleotide, and by the nucleotide in different states of phosphorylation (ATP, ADP.Pi, ADP. Vi, ADP.AlF4, ADP.BeFx, and ADP). Actin isoforms from different species were also compared, and the effect of profilin on the thermal stability of actin was studied. We conclude that the thermal unfolding of G-actin is a three-state process, in which an equilibrium exists between native actin with bound nucleotide and an intermediate free of nucleotide. Actins in the Mg-form were less stable than the Ca-forms, and the stability of the different isoforms decreased in the following order: rabbit skeletal muscle alpha-actin = bovine cytoplasmic gamma-actin > yeast actin > cytoplasmic beta-actin. The activation energies for the thermal unfolding reactions were in the range 200-290 kJ.mol- 1, depending on the bound ligands. Generally, the stability of the actin depended on the degree with which the nucleotide contributed to the connectivity between the two domains of the protein.     

Actin interacts with CCT via discrete binding sites: a binding transition-release model for CCT-mediated actin folding

The chaperones prefoldin and the cytosolic chaperonin CCT-containing TCP-1 (CCT) guide the cytoskeletal protein actin to its native conformation. Performing an alanine scan of actin, we identified discrete recognition determinants for CCT interaction. Interestingly, one of these is similar and functional in the non-homologous protein Cdc20, suggesting that some of the binding information in the CCT target proteins is shared. The information in actin for recognition by CCT and for folding is different, as all but one of the mutants in the recognition determinants are folding-competent. In addition, some other actin mutants remain CCT-arrested and are not released in a native conformation, whereas others do fold but remain bound to CAP. Kinetic experiments provide evidence that CCT-mediated folding of non-native actin occurs in at least two steps, in which initially the recognition determinant 245-249 contacts CCT and the other determinants interact at later stages. Actin mutants that are CCT-arrested demonstrate that some regions neighbouring the recognition determinants are involved in modulating the correct folding transitions of actin on CCT, or its release from this chaperonin. Further, we found that the ATP binding of actin is not a prerequisite for its release, and we suggest that CAP may be involved in charging the nucleotide. Based on the kinetics of CCT binding and folding of actin and actin mutants, we propose a multi-step recognition-transition-release model. This also implies that the currently accepted notion of CCT-mediated actin folding is probably more complex.     

Kinetic barriers to the folding of horse cytochrome C in the reduced state

To determine the kinetic barrier in the folding of horse cytochrome c, a CO-liganded derivative of cytochrome c, called carbonmonoxycytochrome c, has been prepared by exploiting the thermodynamic reversibility of ferrocytochrome c unfolding induced by guanidinium hydrochloride (GdnHCl), pH 7. The CO binding properties of unfolded ferrocytochrome c, studied by 13C NMR and optical spectroscopy, are remarkably similar to those of native myoglobin and isolated chains of human hemoglobin. Equilibrium unfolding transitions of ferrocytochrome c in the presence and the absence of CO observed by both excitation energy transfer from the lone tryptophan to the ferrous heme and far-UV circular dichroism (CD) indicate no accumulation of structural intermediates to a detectable level. Values of thermodynamic parameters obtained by two-state analysis of fluorescence transitions are DeltaG(H2O) = 11.65(+/-1.13) kcal x mol(-1) and C(m) = 3.9(+/-0.1) M GdnHCl in the presence of CO, and DeltaG(H2O)=19.3(+/-0.5) kcal x mol(-1) and C(m) = 5.1(+/-0.1) M GdnHCl in the absence of CO, indicating destabilization of ferrocytochrome c by approximately 7.65 kcal x mol(-1) due to CO binding. The native states of ferrocytochrome c and carbonmonoxycytochrome c are nearly identical in terms of structure and conformation except for the Fe2+-M80 --> Fe2+-CO replacement. Folding and unfolding kinetics as a function of GdnHCl, studied by stopped-flow fluorescence, are significantly different for the two proteins. Both refold fast, but carbonmonoxycytochrome c refolds 2-fold faster (tau = 1092 micros at 10 degrees C) than ferrocytochrome c. Linear extrapolation of the folding rates to the ordinate of the chevron plot projects this value of tau to 407 micros. The unfolding rate of the former in water, estimated by extrapolation, is faster by more than 10 orders of magnitude. Significant differences are also observed in rate-denaturant gradients in the chevron. Formation and disruption of the Fe2+-M80 coordination contact clearly impose high-energy kinetic barriers to folding and unfolding of ferrocytochrome c. The unfolding barrier due to the Fe2+-M80 bond provides sufficient kinetic stability to the native state of ferrocytochrome c to perform its physiological function as an electron donor.     

Effects of sulphate and urea on the stability and reversible unfolding of beta-lactamase from Staphylococcus aureus. Implications for the folding pathway of beta-lactamase

The reversible denaturation by urea of beta-lactamase from Staphylococcus aureus was followed in the presence and absence of ammonium sulphate by circular dichroism studies, difference absorption spectroscopy and measurement of enzyme activity. The multiple unfolding and refolding transitions demonstrate the existence of a thermodynamically stable state of intermediate conformation in equilibrium with the native (N) and fully unfolded (U) states. Its physical properties show that it is identical to the state H found on denaturation by guanidinium chloride. State H is 10.1 (+/-1.5) kJ mol-1 less stable than the native state and 10.1 (+/-1.6) kJ mol-1 more stable than the unfolded state. Ammonium sulphate shifts both the N in equilibrium H and H in equilibrium U transitions to concentrations of urea higher by 5.3 M per mole of sulphate. It has markedly different effects on the thermodynamic stabilities of states N and H, making delta G'N-H, O and delta G'H-U, O more negative by 41 kJ mol and 20 kJ mole, respectively, per mole of ammonium sulphate. The change in equilibrium constant for the N-H transition is reflected almost exclusively in a dramatic change of the unfolding rate constant, which is decreased by a factor of 10(11) on addition of 1.4 M-sulphate. The presence of the substrate benzyl penicillin has little effect on the equilibria or kinetics of the N-H transition. The results are discussed in terms of the nature of the N-H transition and of the ordering of intermediate states on the folding pathway.     

Observation of multistate kinetics during the slow folding and unfolding of barstar.

The kinetics of the slow folding and unfolding reactions of barstar, a bacterial ribonuclease inhibitor protein, have been studied at 23(+/-1) degrees C, pH 8, by the use of tryptophan fluorescence, far-UV circular dichroism (CD), near-UV CD, and transient mixing (1)H nuclear magnetic resonance (NMR) spectroscopic measurements in the 0-4 M range of guanidine hydrochloride (GdnHCl) concentration. The denaturant dependences of the rates of folding and unfolding processes, and of the initial and final values of optical signals associated with these kinetic processes, have been determined for each of the four probes of measurement. Values determined for rates as well as amplitudes are shown to be very much probe dependent. Significant differences in the intensities and rates of appearance and disappearance of several resolved resonances in the real-time one-dimensional NMR spectra have been noted. The NMR spectra also show increasing dispersion of chemical shifts during the slow phase of refolding. The denaturant dependences of rates display characteristic folding chevrons with distinct rollovers under strongly native as well as strongly unfolding conditions. Analyses of the data and comparison of the results obtained with different probes of measurement appear to indicate the accumulation of a myriad of intermediates on parallel folding and unfolding pathways, and suggest the existence of an ensemble of transition states. The energetic stabilities of the intermediates estimated from kinetic data suggest that they are approximately half as stable as the fully folded protein. The slowness of the folding and unfolding processes (tau = 10-333 s) and values of 20.5 (+/-1.4) and 18 (+/-0.5) kcal mol(-)(1) for the activation energies of the slow refolding and unfolding reactions suggest that proline isomerization is involved in these reactions, and that the intermediates accumulate and are therefore detectable because the slow proline isomerization reaction serves as a kinetic trap during folding.     

The pressure-temperature free energy-landscape of staphylococcal nuclease monitored by (1)H NMR

The thermodynamic stability of staphylococcal nuclease was studied against the variation of both temperature and pressure by utilizing (1)H NMR spectroscopy at 750 MHz in 20 mM Mes buffer containing 99.9 % (2)H(2)O, pH 5.3. Equilibrium fractions of folded and unfolded protein species were evaluated with the proton signals of two histidine residues as monitor in the pressure range of 30-3300 bar and in the temperature range of 1.5 degrees C-35 degrees C. From the multi-parameter fit of the experimental data to the Gibbs energy equation expressed as a simultaneous function of pressure and temperature, we determined the compressibility change (Deltabeta), the volume change at 1 bar (DeltaV degrees ) and the expansivity change (Deltaalpha) upon unfolding among other thermodynamic parameters: Deltabeta=0.02(+/-0.003) ml mol(-1) bar(-1); Deltaalpha=1.33(+/-0.2) ml mol(-1) K(-1); DeltaV degrees =-41.9(+/-6. 3) ml mol(-1) (at 24 degrees C); DeltaG degrees =13.18(+/-2) kJ mol(-1) (at 24 degrees C); DeltaC(p)=13.12(+/-2) kJ mol(-1) K(-1); DeltaS degrees =0.32(+/-0.05) kJ mol(-1) K(-1 )(at 24 degrees C). The result yields a three-dimensional free energy surface, i.e. the free energy-landscape of staphylococcal nuclease on the P-T plane. The significantly positive Deltabeta and Deltaalpha values suggest that, in the pressure-denatured state, staphylococcal nuclease forms a loosely packed and fluctuating structure. The slight but statistically significant difference between the unfolding transitions of the His8 and His124 environments is considered to reflect local fluctuations in the native state, leading to pre-melting of the His124 environment prior to the cooperative unfolding of the major part of the protein.     

Isolation and characterization of covalently cross-linked actin dimer

Covalently cross-linked actin dimer was isolated from rabbit skeletal muscle F-actin reacted with phenylenebismaleimide (Knight, P., and Offer, G. (1978) Biochem. J. 175, 1023-1032). The UV spectrum of the purified cross-linked actin dimer, in a nonpolymerizing buffer, was very similar to that of native F-actin and not to the spectrum of G-actin. Cross-linked actin dimer polymerized to filaments that were indistinguishable in the electron microscope from F-actin made from native G-actin and that were similar to native F-actin in their ability to activate the Mg2+-ATPase of myosin subfragment-1. The critical concentrations of polymerization of cross-linked actin dimer in 0.5 mM and 2.0 mM MgCl2, 2 to 4 microM, and 1 to 2 microM, respectively, were similar to the values for native G-actin. Cross-linked actin dimer contained 2 mol of bound nucleotide/mol of dimer. One bound nucleotide exchanged with ATP in solution with a t 1/2 of 55 min and with ADP with a t 1/2 of 5 h. The second bound nucleotide exchanged much more slowly. The more rapidly exchangeable site contained 10 to 15% bound ADP.Pi and 85 to 90% bound ATP while the second site contained much less, if any, bound ADP.Pi. Cross-linked actin dimer had an ATPase activity in 0.5 mM MgCl2 that was 7 times greater than the ATPase activity of native G-actin and that was also stimulated by cytochalasin D. These data are discussed in relation to the possible role of ATP in actin polymerization and function with the speculation that the cross-linked actin dimer may serve simultaneously as a useful model for each of the two different ends of native F-actin.     

Folding of horse cytochrome c in the reduced state

Equilibrium and kinetic folding studies of horse cytochrome c in the reduced state have been carried out under strictly anaerobic conditions at neutral pH, 10 degrees C, in the entire range of aqueous solubility of guanidinium hydrochloride (GdnHCl). Equilibrium unfolding transitions observed by Soret heme absorbance, excitation energy transfer from the lone tryptophan residue to the ferrous heme, and far-UV circular dichroism (CD) are all biphasic and superimposable, implying no accumulation of structural intermediates. The thermodynamic parameters obtained by two-state analysis of these transitions yielded DeltaG(H2O)=18.8(+/-1.45) kcal mol(-1), and C(m)=5.1(+/-0.15) M GdnHCl, indicating unusual stability of reduced cytochrome c. These results have been used in conjunction with the redox potential of native cytochrome c and the known stability of oxidized cytochrome c to estimate a value of -164 mV as the redox potential of the unfolded protein. Stopped-flow kinetics of folding and unfolding have been recorded by Soret heme absorbance, and tryptophan fluorescence as observables. The refolding kinetics are monophasic in the transition region, but become biphasic as moderate to strongly native-like conditions are approached. There also is a burst folding reaction unobservable in the stopped-flow time window. Analyses of the two observable rates and their amplitudes indicate that the faster of the two rates corresponds to apparent two-state folding (U<-->N) of 80-90 % of unfolded molecules with a time constant in the range 190-550 micros estimated by linear extrapolation and model calculations. The remaining 10-20 % of the population folds to an off-pathway intermediate, I, which is required to unfold first to the initial unfolded state, U, in order to refold correctly to the native state, N (I<-->U<-->N). The slower of the two observable rates, which has a positive slope in the linear functional dependence on the denaturant concentration indicating that an unfolding process under native-like conditions indeed exists, originates from the unfolding of I to U, which rate-limits the overall folding of these 10-20 % of molecules. Both fast and slow rates are independent of protein concentration and pH of the refolding milieu, suggesting that the off-pathway intermediate is not a protein aggregate or trapped by heme misligation. The nature or type of unfolded-state heme ligation does not interfere with refolding. Equilibrium pH titration of the unfolded state yielded coupled ionization of the two non-native histidine ligands, H26 and H33, with a pK(a) value of 5.85. A substantial fraction of the unfolded population persists as the six-coordinate form even at low pH, suggesting ligation of the two methionine residues, M65 and M80. These results have been used along with the known ligand-binding properties of unfolded cytochrome c to propose a model for heme ligation dynamics. In contrast to refolding kinetics, the unfolding kinetics of reduced cytochrome c recorded by observation of Soret absorbance and tryptophan fluorescence are all slow, simple, and single-exponential. In the presence of 6.8 M GdnHCl, the unfolding time constant is approximately 300(+/-125) ms. There is no burst unfolding reaction. Simulations of the observed folding-unfolding kinetics by numerical solutions of the rate equations corresponding to the three-state I<-->U<-->N scheme have yielded the microscopic rate constants.     

Analysis of folding and unfolding reactions of cytochrome b5

The guanidine hydrochloride- (GuHCl-) induced unfolding and refolding of a recombinant domain of bovine microsomal cytochrome b(5) containing the first 104 amino acid residues has been characterized by both transient and equilibrium spectrophotometric methods. The soluble domain is reversibly unfolded and the equilibrium reaction may be monitored by changes in absorbance and fluorescence that accompany denaturation of the native protein. Both probes reveal a single cooperative transition with a midpoint at 3 M GuHCl and lead to a value for the protein stability (DeltaG(uw)) of 26.5 kJ mol(-1). This stability is much higher than that reported for the corresponding form of the apoprotein (approximately 7 kJ mol(-1)). Transient changes in fluorescence and absorbance during protein unfolding exhibit biphasic profiles. A fast phase occupying approximately 30% of the total amplitude is observed at high denaturant concentrations and becomes the dominant process within the transition region. The rates associated with each process show a linear dependency on GuHCl concentration, and at zero denaturant concentration the unfolding rates (k(uw)) are 4.5 x 10(-5) s(-1) and 5.2 x 10(-6) s(-1) at 25 degrees C. The pattern of unfolding is not correlated with covalent heterogeneity, since a wide range of variants and site-directed mutants exhibit identical profiles, nor is the unfolding correlated with cis-trans Pro isomerization in the native state. In comparison with the apo form of cytochrome b(5), the kinetics of refolding and unfolding are more complex and exhibit very different transition states. The data support a model for unfolding in which heme-protein interactions give rise to two discernible rates of unfolding. From an analysis of the activation parameters associated with each process it is established that two structurally similar transition states differing by less than 5 kJ mol(-1) exist in the unfolding reaction. Protein refolding exhibits monophasic kinetics but with distinct curvature apparent in plots of ln k(obs) versus denaturant concentration. The data are interpreted in terms of alternative routes for protein folding in which a "fast track" leads to the rapid ordering of structure around Trp26 for refolding while a slower route requires additional reorganization around the hydrophobic core.     

Selective stabilization of a partially unfolded protein by a metabolite

When proteins fold in vivo, the intermediates that exist transiently on their folding pathways are exposed to the potential interactions with a plethora of metabolites within the cell. However, these potential interactions are commonly ignored. Here, we report a case in which a ubiquitous metabolite interacts selectively with a nonnative conformation of a protein and facilitates protein folding and unfolding process. From our previous proteomics study, we have discovered that Escherichia coli glyceraldehyde-3-phosphate dehydrogenase (GAPDH), which is not known to bind ATP under native conditions, is apparently destabilized in the presence of a physiological concentration of ATP. To decipher the origin of this surprising effect, we investigated the thermodynamics and kinetics of folding and unfolding of GAPDH in the presence of ATP. Equilibrium unfolding of the protein in urea showed that a partially unfolded equilibrium intermediate accumulates in the presence of ATP. This intermediate has a quaternary structure distinct from the native protein. Also, ATP significantly accelerates the unfolding of GAPDH by selectively stabilizing a transition state that is distinct from the native state of the protein. Moreover, ATP also significantly accelerates the folding of GAPDH. These results demonstrate that ATP interacts specifically with a partially unfolded form of GAPDH and affects the kinetics of folding and unfolding of this protein. This unusual effect of ATP on the folding of GAPDH implies that endogenous metabolites may facilitate protein folding in vivo by interacting with partially unfolded intermediates.     

Quantitative actin folding reactions using yeast CCT purified via an internal tag in the CCT3/gamma subunit

The eukaryotic cytosolic chaperonin CCT is an essential ATP-dependent protein folding machine whose action is required for folding the cytoskeletal proteins actin and tubulin, and a small number of other substrates, including members of the WD40-propellor repeat-containing protein family. An efficient purification protocol for CCT from Saccharomyces cerevisiae has been developed. It uses the calmodulin binding peptide as an affinity tag in an internal loop in the apical domain of the CCT3 subunit, which is predicted to be located on the outside of the double-ring assembly. This purified yeast CCT was used for a novel quantitative actin-folding assay with human beta-actin or yeast ACT1p protein folding intermediates, Ac(I), pre-synthesised in an Escherichia coli translation system. The formation of native actin follows approximately a first-order reaction with a rate constant of about 0.03 min(-1). Yeast CCT catalyses the folding of yeast ACT1p and human beta-actin with nearly identical rate constants and yields. The results from this controlled CCT-actin folding assay are consistent with a model where CCT and Ac(I) are in a binding pre-equilibrium with a rate-limiting binding step, followed by a faster ATP-driven processing to native actin. In this pure in vitro system, the human beta-actin mutants, D244S and G150P, show impaired folding behaviour in the manner predicted by our sequence-specific recognition model for CCT-actin interaction.     

Correlation between mutational destabilization of phage T4 lysozyme and increased unfolding rates

The thermodynamics and kinetics of unfolding of 28 bacteriophage T4 lysozyme variants were compared by using urea gradient gel electrophoresis. The mutations studied cause a variety of sequence changes at different residues throughout the polypeptide chain and result in a wide range of thermodynamic stabilities. A striking relationship was observed between the thermodynamic and kinetic effects of the amino acid replacements: All the substitutions that destabilized the native protein by 2 kcal/mol or more also increased the rate of unfolding. The observed increases in unfolding rate corresponded to a decrease in the activation energy of unfolding (delta Gu) at least 35% as large as the decrease in thermodynamic stability (delta Gu). Thus, the destabilizing lesions bring the free energy of the native state closer to that of both the unfolded state and the transition state for folding and unfolding. Since a large fraction of the mutational destabilization is expressed between the transition state and the native conformation, the changes in folding energetics cannot be accounted for by effects on the unfolded state alone. The results also suggest that interactions throughout much of the folded structure are altered in the formation of the transition state during unfolding.     

Folding intermediates of a model three-helix bundle protein. Pressure and cold denaturation studies

The stability and equilibrium unfolding of a model three-helix bundle protein, alpha(3)-1, by guanidine hydrochloride (GdnHCl), hydrostatic pressure, and temperature have been investigated. The combined use of these denaturing agents allowed detection of two partially folded states of alpha(3)-1, as monitored by circular dichroism, intrinsic fluorescence emission, and fluorescence of the hydrophobic probe bis-ANS (4,4'-dianilino-1,1'-binaphthyl-5,5'-disulfonic acid). The overall free-energy change for complete unfolding of alpha(3)-1, determined from GdnHCl unfolding data, is +4.6 kcal/mol. The native state is stabilized by -1.4 kcal/mol relative to a partially folded pressure-denatured intermediate (I(1)). Cold denaturation at high pressure gives rise to a second partially (un)folded conformation (I(2)), suggesting a significant contribution of hydrophobic interactions to the stability of alpha(3)-1. The free energy of stabilization of the native-like state relative to I(2) is evaluated to be -2.5 kcal/mol. Bis-ANS binding to the pressure- and cold-denatured states indicates the existence of significant residual hydrophobic structure in the partially (un)folded states of alpha(3)-1. The demonstration of folding intermediates of alpha(3)-1 lends experimental support to a number of recent protein folding simulation studies of other three-helix bundle proteins that predicted the existence of such intermediates. The results are discussed in terms of the significance of de novo designed proteins for protein folding studies.     

Unfolding thermodynamics of Trp-cage, a 20 residue miniprotein, studied by differential scanning calorimetry and circular dichroism spectroscopy

Small proteins provide convenient models for computational studies of protein folding and stability, which are usually compared with experimental data. Until recently, the unfolding of Trp-cage was considered to be a two-state process. However, no direct experimental evidence for this has been presented, and in some cases, the contrary has been suggested. To elucidate a detailed unfolding mechanism, we studied the thermodynamics of unfolding of Trp-cage by differential scanning calorimetry (DSC) and circular dichroism (CD) spectroscopy. The observation that at low temperatures only approximately 90-95% of Trp-cage exists in the native conformation presented an analytical challenge. Nevertheless, it was found that the DSC and CD data can be fitted simultaneously to the same set of thermodynamic parameters. The major uncertainty in such a global fit is the heat capacity change upon unfolding, DeltaCp. This can be circumvented by obtaining DeltaCp directly from the difference between heat capacity functions of the native and unfolded states. Using such an analysis it is shown that Trp-cage unfolding can be represented by a two-state model with the following thermodynamic parameters: Tm = 43.9 +/- 0.8 degrees C, DeltaH(Tm) = 56 +/- 2 kJ/mol, DeltaCp = 0.3 +/- 0.1 kJ/(mol.K). Using these thermodynamic parameters it is estimated that Trp-cage is marginally stable at 25 degrees C, DeltaG(25 degrees C) = 3.2 +/- 0.2 kJ/mol, which is only 30% more than the thermal fluctuation energy at this temperature.     

Evolutionally conserved intermediates between ubiquitin and NEDD8

The investigation of common structural motifs provides additional information on why proteins conserve similar topologies yet may have non-conserved amino acid sequences. Proteins containing the ubiquitin superfold have similar topologies, although the sequence conservation is rather poor. Here, we present novel similarities and differences between the proteins ubiquitin and NEDD8. They have 57% identical sequence, almost identical backbone topology and similar functional strategy, although their physiological functions are mutually different. Using variable pressure NMR spectroscopy, we found that the two proteins have similar conformational fluctuation in the evolutionary conserved enzyme-binding region and contain a structurally similar locally disordered conformer (I) in equilibrium with the basic folded conformer (N). A notable difference between the two proteins is that the equilibrium population of I is far greater for NEDD8 (DeltaG(0)(NI)<5 kJ/mol) than for ubiquitin (DeltaG(0)(NI)=15.2(+/-1.0) kJ/mol), and that the tendency for overall unfolding (U) is also far higher for NEDD8 (DeltaG(0)(NU)=11.0(+/-1.5) kJ/mol) than for ubiquitin (DeltaG(0)(NU)=31.3(+/-4.7) kJ/mol). These results suggest that the marked differences in thermodynamic stabilities of the locally disordered conformer (I) and the overall unfolding species (U) are a key to determine the functional differences of the two structurally similar proteins in physiology.     

Temperature dependence and Arrhenius activation energy of F-actin velocity generated in vitro by skeletal myosin.

The effect of temperature on the velocity of rhodamine phalloidin-labelled F-actin moving in vitro on rabbit skeletal myosin has been studied. Translating actin filaments were visualized by epi-fluorescence in an inverted microscope, equipped with temperature control (+/- 0.2 K) of the stage and objective. Images were recorded in real time at magnifications of 400x or 160x by an intensified CCD camera on video tape. Motion of individual filaments was tracked by hand and velocities determined using frame times recorded simultaneously on the video tape. Velocity changed from 12 microns per second at 42 degrees C to 11 nm per second at 3 degrees C. The Arrhenius plot is non-linear, with the data following a cubic regression curve with no evident breaks or jumps. Data taken over the temperature range from single preparations followed the same curve for both heating and cooling; this indicates reversibility and absence of hysteresis. A hyperbolic model that smoothly translates with temperature between two asymptotic activation energies fits the data above 7 degrees C: these energies are 50(+/- 5) kJ per mole (Q10 = 1.9) at high temperatures and 289(+/- 29) kJ per mole (Q10 = 76.5) at low temperature with a transition temperature of 15.4(+/- 0.6) degrees C. These values are compared with other measurements made in vitro, in solution studies and on muscle fibres. An Arrhenius activation energy of 50 kJ per mole and a transition temperature of 15 degrees C are consistent with previous determinations but 289 kJ per mole is significantly greater than has been seen at low temperatures in other systems. This may indicate a different rate-limiting step in the kinetics of skeletal myosin driving actin filaments in vitro below 15 degrees C. Current determinations of the myosin "step-size" assume that the actin velocity is determined by the rate of ATP hydrolysis; the data confirm similar activation energies above 20 degrees C but they show that the temperature dependencies and activation energies are different at lower temperatures, implying uncoupling of the two processes.     

The cytosolic class II chaperonin CCT recognizes delineated hydrophobic sequences in its target proteins

The nonhomologous proteins actin and alpha- and beta-tubulin need the assistance of the cytosolic chaperonin containing TCP-1 (CCT) to reach their correct native state, and their folding requires a transient binary complex formation with CCT. We show that separate or combined deletion of three delineated hydrophobic sequences in actin disturbs the interaction with CCT. These sites are situated between residues 125-179, 244-285, and 340-375. Also, alpha- and beta-tubulin contain at least one recognition region, and intriguingly, it has a similar distribution of hydrophobic residues as region 244-285 in actin. Internal deletion of the sites in actin favor a model for cooperative binding of target proteins to CCT. Peptide mimetics, representing the binding regions, inhibit target polypeptide binding to CCT, suggesting that actin and tubulin contact similar CCT subunits. In addition, we show that actin recognition by class II chaperonins is different from that by class I.     

Folding kinetics of the all-beta-sheet protein human basic fibroblast growth factor, a structural homolog of interleukin-1beta

The refolding and unfolding kinetics of the all-beta-sheet protein human basic fibroblast growth factor (hFGF-2) were studied by fluorescence spectroscopy. The kinetics of the unfolding transition are monophasic. The refolding reaction at high and low guanidinium chloride (GdmCl) concentrations is best described by mono- and biphasic folding, respectively. Refolding and unfolding of hFGF-2 (155 amino acids) is very slow compared with other non-disulfide-bonded monomeric proteins of similar size. For example, the rate constant for unfolding at 4.5 mol.liter(-1) GdmCl is 0.006 s(-1), and the refolding rate constants at 0.4 mol.liter(-1) GdmCl are 0.01 s(-1) and 0.0009 s(-1) (15 degrees C, pH 7.0). A characterization of the thermodynamic nature of the folding process using transition state theory revealed that the slow refolding is almost exclusively controlled by entropic factors, namely the strong loss of conformational freedom during refolding. The rate of the slow unfolding kinetics is mainly (and at low denaturant concentrations exclusively) controlled by the large positive change in enthalpy. hFGF-2 shows similar slow folding kinetics to that of its structural homolog interleukin-1beta. Since both proteins show very little sequence identity, it is suggested that their slow folding kinetics are determined by the complex beta-sheet arrangement of the native molecules.