Denatured state thermodynamics: residual structure, chain stiffness and scaling factors

A set of nine variants of yeast iso-1-cytochrome c with zero or one surface histidine have been engineered such that the N-terminal amino group is acetylated in vivo. N-terminal acetylation has been confirmed by mass spectral analysis of intact and proteolytically digested protein. The histidine-heme loop-forming equilibrium, under denaturing conditions (3 M guanidine hydrochloride), has been measured by pH titration providing an observed pK(a), pK(a)(obs), for each variant. N-terminal acetylation prevents the N-terminal amino group-heme binding equilibrium from interfering with measurements of histidine-heme affinity. Significant deviation is observed from the linear dependence of pK(a)(obs) on the log of the number of monomers in the loop formed, expected for a random coil denatured state. The maximum histidine-heme affinity occurs for a loop size of 37 monomers. For loop sizes of 37-83 monomers, histidine-heme pK(a)(obs) values are consistent with a scaling factor of -4.2+/-0.3. This value is much larger than the scaling factor of -1.5 for a freely jointed random coil, which is commonly used to represent the conformational properties of protein denatured states. For loop sizes of nine to 22 monomers, chain stiffness is likely responsible for the decreases in histidine-heme affinity relative to a loop size of 37. The results are discussed in terms of residual structure and sequence composition effects on the conformational properties of the denatured states of proteins.     

Kinetics of loop formation and breakage in the denatured state of iso-1-cytochrome c

The earliest events in protein folding involve the formation of simple loops. Observing the rates of loop closure under denaturing conditions can provide direct insight into the relative probability and sequence determinants for formation of loops of different sizes. The persistence of these initial contacts is equally important for efficient folding, so measurement of rates of loop breakage under denaturing conditions is also essential. We have used stopped-flow and continuous-flow methods to measure the rates of histidine-heme loop formation and breakage in the denatured state of iso-1-cytochrome c (in the presence of 3 M guanidine HCl). The data indicate that the mechanism for forming loops is a two-step process, the first step being the deprotonation of the histidine, and the second step being the binding of the histidine to the heme. This mechanism makes it possible to extract both the rate constants of formation, k(f), and breakage, k(b), of loops from the pH dependence of the observed rate constant, k(obs). To determine the dependence of k(f) and k(b) on loop size, we have carried out kinetic measurements for seven single surface histidine variants of iso-1-cytochrome c. A scaling factor (the dependence of k(f) on log[loop size]) of approximately -1.8 is observed for loop formation, similar to that observed in other systems. The magnitude of k(b) varies from 30 s(-1) to 300 s(-1), indicating that the stability of different loops varies considerably. The implications of the kinetics of loop formation and breakage in the denatured state for the mechanism of protein folding are discussed.     

The pH dependence of the reversible unfolding of ovalbumin A1 by guanidine hydrochloride.

The pH dependence of the reversible guanidine hydrochloride denaturation of the major fraction of ovalbumin (ovalbumin A1) was studied by a viscometric method in the pH range 1-7, at 25 degrees C and at six different denaturant concentrations (1.5-2.6 M). At any denaturant concentrationa reduction in pH favoured the transition from the native to the denatured state. The latter was essentially 'structureless', as revealed by the fact that the reduced viscosity of the acid and guanidine hydrochloride denatured state of ovalbumin A1 (obtained at different denaturant concentrations in acidic solutions) was measured (at a protein concentration of 3.8 mg/ml) to be 29.2 ml/g which is identical to that found in 6 M guanidine hydrochloride wherein the protein behaves as a cross-linked random coil. A quantitative analysis of the results on the pH dependence of the equilibrium constant for the denaturation process showed that on denaturation the intrinsic pK of two carboxyl groups in ovalbumin A1 went up from 3.1 in the native state to 4.4 in the denatured state of the protein.     

A semiflexible polymer model applied to loop formation in DNA hairpins

A statistical mechanical "zipper" model is applied to describe the equilibrium melting of short DNA hairpins with poly(dT) loops ranging from 4 to 12 bases in the loop. The free energy of loop formation is expressed in terms of the persistence length of the chain. This method provides a new measurement of the persistence length of single-stranded DNA, which is found to be approximately 1.4 nm for poly(dT) strands in 100 mM NaCl. The free energy of the hairpin relative to the random coil state is found to scale with the loop size with an apparent exponent of > or = 7, much larger than the exponent of approximately 1.5-1.8 expected from considerations of loop entropy alone. This result indicates a strong dependence of the excess stability of the hairpins, from stacking interactions of the bases within the loop, on the size of the loop. We interpret this excess stability as arising from favorable hydrophobic interactions among the bases in tight loops and which diminish as the loops get larger. Free energy profiles along a generalized reaction coordinate are calculated from the equilibrium zipper model. The transition state for hairpin formation is identified as an ensemble of looped conformations with one basepair closing the loop, and with a lower enthalpy than the random coil state. The equilibrium model predicts apparent activation energy of approximately -11 kcal/mol for the hairpin closing step, in remarkable agreement with the value obtained from kinetics measurements.     

Correspondence between anomalous m- and DeltaCp-values in protein folding

Proteins folding according to a classical two-state system characteristically show V-shaped chevron plots. We have previously interpreted the symmetrically curved chevron plot of the protein U1A as denaturant-dependent movements in the position of the transition state ensemble (TSE). S6, a structural analog of U1A, shows a classical V-shaped chevron plot indicative of straightforward two-state kinetics, but the mutant LA30 has a curved unfolding limb, which is most consistent with TSE mobility. The kinetic m-values (derivatives of the rate constants with respect to denaturant concentration) in themselves depend on denaturant concentration. To obtain complementary information about putative mobile TSEs, we have carried out a thermodynamic analysis of the three proteins, based on data for refolding and unfolding over the range 10 degrees C to 70 degrees C. The data at all temperatures can be fitted to two-state model systems. Importantly, for all three proteins the activation heat capacities are, within error, identical to the heat capacities measured in independent experiments under equilibrium conditions. Although the equilibrium heat capacities are essentially invariant with regard to denaturant concentration, the activation heat capacities, similar to the structurally equivalent kinetic m-values, show marked denaturant dependence. Furthermore, the values of beta++ at different denaturant concentrations measured by m-values and by heat capacity values are very similar. These observations are consistent with significant transition state movements within the framework of two-state folding. The basis for TSE movement appears to be enthalpic rather than entropic, suggesting that the binding energy of denaturant-protein interactions is a major determinant of the response of energy landscape contours to changing environments.     

Manifestations of native topology in the denatured state ensemble of Rhodopseudomonas palustris cytochrome c'

To provide insight into the role of local sequence in the nonrandom coil behavior of the denatured state, we have extended our measurements of histidine-heme loop formation equilibria for cytochrome c' to 6 M guanidine hydrochloride. We observe that there is some reduction in the scatter about the best fit line of loop stability versus loop size data in 6 M versus 3 M guanidine hydrochloride, but the scatter is not eliminated. The scaling exponent, ν(3), of 2.5 ± 0.2 is also similar to that found previously in 3 M guanidine hydrochloride (2.6 ± 0.3). Rates of histidine-heme loop breakage in the denatured state of cytochrome c' show that some histidine-heme loops are significantly more persistent than others at both 3 and 6 M guanidine hydrochloride. Rates of histidine-heme loop formation more closely approximate random coil behavior. This observation indicates that heterogeneity in the denatured state ensemble results mainly from contact persistence. When mapped onto the structure of cytochrome c', the histidine-heme loops with slow breakage rates coincide with chain reversals between helices 1 and 2 and between helices 2 and 3. Molecular dynamics simulations of the unfolding of cytochrome c' at 498 K show that these reverse turns persist in the unfolded state. Thus, these portions of the primary structure of cytochrome c' set up the topology of cytochrome c' in the denatured state, predisposing the protein to fold efficiently to its native structure.     

Equilibrium and kinetics of the unfolding of alpha-lactalbumin by guanidine hydrochloride (IV): dependence of the N equilibrium A transconformation on the temperature.

The reversible unfolding from the native (N) state to the acid (A) state of alpha-lactalbumin by guanidine-HCl (0.8-2.0 M) was studied at 10-35 degrees C by means of difference spectra and pH-jump measurements. At each temperature, all points plotted as the logarithmic equilibrium constant log KNA of the N equilibrium A process against pH could fall on a curve independent of the denaturant concentration by shifting each point along the log KNA axis, where the shift factor f did not depend on temperature. Moreover, by shifting the points at each temperature along the log (KNA/f) axis, a master curve, independent of both temperature and the denaturant concentration, could be obtained for the pH-dependence of log KNA. From the dependence of the logarithmic rate constants on pH, master curves independent of both temperature and the denaturant concentration could also be made for the N leads to A and the A leads to A processes, where A mean the activated state. The results show the two-state character of the N equilibrium A process. The enthalpy changes and the differences in heat capacity for the N equilibrium A, N equilibrium A and A equilibrium A processes were determined from the accurate measurements of temperature dependence of the unfolding at pH 4.3 and 1.0 M guanidine-HCl. The results show that the disruption of hydrophobic interaction is caused mainly in the A leads to A process, while most of the changes in the pK values of the ionizing groups are caused in the N leads to A process.     

Effects of Ca(2+)-activated calmodulin on neuronal nitric oxide synthase reductase activity and binding of substrates: pH dependence of kinetic parameters.

The pH dependence of basal and calmodulin- (CaM-) stimulated neuronal nitric oxide synthase (nNOS) reduction of 2,6-dichloroindophenol (DCIP) and cytochrome c(3+) was investigated. The wave-shaped log V versus pH profile revealed that optimal DCIP reduction occurred when a group, pK(a) of 7.6-7.8, was ionized. The (V/K)(NADPH) and (V/K)(DCIP) versus pH profiles increased with the protonation of a group with a pK(a) of 6.5 or 5.9 and the ionization of two groups with the same pK(a) of 7.5 or 7.0, respectively. (V/K)(DCIP) decreased with the ionization of a group, pK(a) of 9.0. Similar V, (V/K)(NADPH), and (V/K)(DCIP) versus pH profiles for DCIP reduction were obtained with and without CaM, indicating that CaM does not influence ionizable groups involved in catalysis or substrate binding. In contrast, CaM affected the pH dependence of cytochrome c(3+) reduction. The wave-shaped log V versus pH profile for basal cytochrome c(3+) reduction revealed that ionization of a group, pK(a) of 8.6, increased catalysis. Log V for CaM-stimulated cytochrome c(3+) reduction displayed a bell-shaped pH dependence with the protonation of a group with a pK(a) of 6.4 and the ionization of a group with a pK(a) of 9.3, resulting in a loss of activity. The log(V/K)(cytc) versus pH profiles with and without CaM were bell-shaped with the ionization of a group at pK(a) of 7.1 or 7.6 (CaM) or pK(a) of 9.4 or 9.6 (CaM), increasing and decreasing (V/K)(cytc). These results suggest that CaM may change the nature of the rate-limiting catalytic steps or ionizable groups involved in cytochrome c(3+) reduction.     

Thermodynamics of Loop Formation in the Denatured State of Rhodopseudomonas palustris Cytochrome c′: Scaling Exponents and the Reconciliation Problem

The observation that denatured proteins yield scaling exponents, ν, consistent with random-coil behavior and yet can also have pockets of residual or nonrandom structure has been termed the “reconciliation problem”. To provide greater insight into the denatured state of a foldable sequence, we have measured histidine-heme loop formation equilibria in the denatured state of a class II c-type cytochrome, cytochrome c′ from Rhodopseudomonas palustris. We have prepared a series of variants that provide His-heme loop stabilities, pK_loop(His), for loop sizes ranging from 10 to 111 residues at intervals of 7 to 11 residues along the sequence of the protein. We observe a scaling exponent for loop formation, ν₃, of 2.5 ± 0.3. Theoretical values for ν₃ range from 1.8 to 2.4; thus, the observed ν₃ is consistent with random-coil behavior. However, in contrast to data for loop formation as a function of loop size obtained with peptides of homogeneous sequence, we observe considerable scatter about the linear dependence of loop stability on loop size. Thus, foldable sequences behave very differently from homogeneous peptide sequences. The observed scatter suggests that there is considerable variation in the conformational properties along the backbone of a foldable sequence, consistent with alternating compact and extended regions. With regard to the reconciliation problem, it is evident that a scaling exponent consistent with a random coil is necessary but not sufficient to demonstrate random-coil behavior.     

Large loop conformation sampling using the activation relaxation technique, ART-nouveau method

We present an adaptation of the ART-nouveau energy surface sampling method to the problem of loop structure prediction. This method, previously used to study protein folding pathways and peptide aggregation, is well suited to the problem of sampling the conformation space of large loops by targeting probable folding pathways instead of sampling exhaustively that space. The number of sampled conformations needed by ART nouveau to find the global energy minimum for a loop was found to scale linearly with the sequence length of the loop for loops between 8 and about 20 amino acids. Considering the linear scaling dependence of the computation cost on the loop sequence length for sampling new conformations, we estimate the total computational cost of sampling larger loops to scale quadratically compared to the exponential scaling of exhaustive search methods.     

IR spectra of cytochrome c denatured with deuterated guanidine hydrochloride show increase in beta sheet

Attenuated total reflectance Fourier transform IR (ATR-FTIR) spectra are obtained for horse heart ferricytochrome c in solutions of 0-7M guanidine hydrochloride and deuterated guanidine hydrochloride. Substitutions of deuterium for hydrogen in both the denaturant and protein provide resolvable amide I spectra over a wide range of denaturant concentrations. Deuteration enhances the ability to measure the true protein IR spectrum in the amide I region in which the secondary structure can be deduced, because spectra in D(2)O are less prone to spectral distortion upon background denaturant subtraction than spectra in H(2)O. Other investigators studying equilibrium unfolded cytochrome c were limited to guanidine concentrations below 3.0M because of detector saturation. Detector saturation is avoided with the use of ATR-FTIR spectroscopy, allowing one to obtain protein spectra at high denaturant concentrations. Second derivative spectra of samples show reductions in alpha helix and increases in beta sheet at high denaturant concentrations, contrary to expectations of finding primarily a random coil secondary structure. Using this new technique, the protein was estimated to consist of 51% beta sheet and only 15% random coil in the presence of 6.6M deuterated guanidine hydrochloride.     

Thermal and urea-induced unfolding of the marginally stable lac repressor DNA-binding domain: a model system for analysis of solute effects on protein processes

Thermodynamic and structural evidence indicates that the DNA binding domains of lac repressor (lacI) exhibit significant conformational adaptability in operator binding, and that the marginally stable helix-turn-helix (HTH) recognition element is greatly stabilized by operator binding. Here we use circular dichroism at 222 nm to quantify the thermodynamics of the urea- and thermally induced unfolding of the marginally stable lacI HTH. Van't Hoff analysis of the two-state unfolding data, highly accurate because of the large transition breadth and experimental access to the temperature of maximum stability (T(S); 6-10 degrees C), yields standard-state thermodynamic functions (deltaG(o)(obs), deltaH(o)(obs), deltaS(o)(obs), deltaC(o)(P,obs)) over the temperature range 4-40 degrees C and urea concentration range 0 相似文献   

Speciation study of the anti-inflammatory drug tenoxicam (Htenox) with Cu(II): X-ray crystal structure of [Cu(tenox)(2)(py)(2)].EtOH

A speciation study was carried out in aqueous solution of the anti-inflammatory drug tenoxicam (Htenox), under quasi-physiological conditions (temperature of 37 degrees C and ionic strength 0.15 M NaCl) in order to determine the acidity constants from spectrophotometric studies, the pK(a) values found being pK(1)=1.143+/-0.008 and pK(2)=4.970+/-0.004. Subsequently, the spectrophotometrical speciation of the different complexes of Cu(II) with the drug was performed under the same conditions of temperature and ionic strength, observing the formation of Cu(Htenox)(2)(2+) with log beta(212)=20.05+/-0.01, Cu(tenox)(2) with log beta(012)=13.6+/-0.1, Cu(Htenox)(2+) with log beta(111)=10.52+/-0.08, as well as Cu(tenox)(+) with log beta(011)=7.0+/-0.2, all of them in solution, and solid species Cu(tenox)(2)(s) with an estimated value of log beta(012)(s) approximately 18.7. The crystalline structure of the complex [Cu(tenox)(2)(py)(2)]. EtOH, was also determined, and it was observed that tenoxicam employs the oxygen of the amide group and the pyridyl nitrogen to bond to the cation.     

Chemical denaturation: potential impact of undetected intermediates in the free energy of unfolding and m-values obtained from a two-state assumption.

The chemical unfolding transition of a protein was simulated, including the presence of an intermediate (I) in equilibrium with the native (N) and unfolded (U) states. The calculations included free energies of unfolding, DeltaGuw, in the range of 1.4 kcal/mol to 10 kcal/mol and three different global m-values. The simulations included a broad range of equilibrium constants for the N left arrow over right arrow I process. The dependence of the N <--> I equilibrium on the concentration of denaturant was also included in the simulations. Apparent DeltaGuw and m-values were obtained from the simulated unfolding transitions by fitting the data to a two-state unfolding process. The potential errors were calculated for two typical experimental situations: 1) the unfolding is monitored by a physical property that does not distinguish between native and intermediate states (case I), and 2) the physical property does not distinguish between intermediate and unfolded states (case II). The results obtained indicated that in the presence of an intermediate, and in both experimental situations, the free energy of unfolding and the m-values could be largely underestimated. The errors in DeltaGuw and m-values do not depend on the m-values that characterize the global N <--> U transition. They are dependent on the equilibrium constant for the N <--> I transition and its characteristic m1-value. The extent of the underestimation increases for higher energies of unfolding. Including no random error in the simulations, it was estimated that the underestimation in DeltaGuw could range between 25% and 35% for unfolding transitions of 3-10 kcal/mol (case I). In case II, the underestimation in DeltaGuw could be even larger than in case I. In the same energy range, a 50% error in the m-value could also take place. The fact that most of the mutant proteins are characterized by both a lower m-value and a lower stability than the wild-type protein suggests that in some cases the results could have been underestimated due to the application of the two-state assumption.     

Intrinsically disordered structure of Bacillus pasteurii UreG as revealed by steady-state and time-resolved fluorescence spectroscopy

UreG is an essential protein for the in vivo activation of urease. In a previous study, UreG from Bacillus pasteurii was shown to behave as an intrinsically unstructured dimeric protein. Here, intrinsic and extrinsic fluorescence experiments were performed, in the absence and presence of denaturant, to provide information about the form (fully folded, molten globule, premolten globule, or random coil) that the native state of BpUreG assumes in solution. The features of the emission band of the unique tryptophan residue (W192) located on the C-terminal helix, as well as the rate of bimolecular quenching by potassium iodide, indicated that, in the native state, W192 is protected from the aqueous polar solvent, while upon addition of denaturant, a conformational change occurs that causes solvent exposure of the indole side chain. This structural change, mainly affecting the C-terminal helix, is associated with the release of static quenching, as shown by resolution of the decay-associated spectra. The exposure of protein hydrophobic sites, monitored using the fluorescent probe bis-ANS, indicated that the native dimeric state of BpUreG is disordered even though it maintains a significant amount of tertiary structure. ANS fluorescence also indicated that, upon addition of a small amount of GuHCl, a transition to a molten globule state occurs, followed by formation of a pre-molten globule state at a higher denaturant concentration. The latter form is resistant to full unfolding, as also revealed by far-UV circular dichroism spectroscopy. The hydrodynamic parameters obtained by time-resolved fluorescence anisotropy at maximal denaturant concentrations (3 M GuHCl) confirmed the existence of a disordered but stable dimeric protein core. The nature of the forces holding together the two monomers of BpUreG was investigated. Determination of free thiols in native or denaturant conditions, as well as light scattering experiments in the absence and presence of dithiothreitol as a reducing agent, under native or denaturing conditions, indicates that a disulfide bond, involving the unique conserved cysteine C68, is present under native conditions and maintained upon addition of denaturant. This covalent bond is therefore important for the stabilization of the dimer under native conditions. The intrinsically disordered structure of UreG is discussed with respect to the role of this protein as a chaperone in the urease assembly system.     

Ionization of amino acid residues involved in the catalytic mechanism of aspartate transcarbamoylase.

The chemical and kinetic mechanisms of the reaction catalyzed by the catalytic trimer of aspartate transcarbamoylase have been examined. The variation of the kinetic parameters with pH indicated that at least four ionizing amino acid residues are involved in substrate binding and catalysis. The pH dependence of K(ia) for carbamoyl phosphate and the K(i) for N-(phosphonoacetyl)-L- aspartate revealed that a protonated residue with a pK value of 9.0 is required for the binding of carbamoyl phosphate. However, the variation with pH of K(i) for succinate, a competitive inhibitor of aspartate, and for cysteine sulfinate, a slow substrate, showed that a single residue with a pK value of 7.3 must be protonated for binding these analogues and, by inference, aspartate. The profile of log V against pH displayed a decrease in reaction rate at low and high pH, suggesting that two groups associated with the Michaelis complex, a deprotonated residue with a pK value of 7.2 and a protonated group with a pK value of 9.5, are involved in catalysis. By contrast, the catalytically productive form of the enzyme-carbamoyl phosphate complex, as illustrated in the bell-shaped pH dependence of log (V/K)(asp), is one in which a residue with a pK value of 7.0 must be protonated while a group with a pK value of 9.1 is deprotonated. This interpretation is supported by the results from the temperature dependence of the V and V/K profiles and from the pH dependence of pK(i) for the aspartate analogues.(ABSTRACT TRUNCATED AT 250 WORDS)     

Electrostatic forces at helix-coil boundaries in DNA

The Tm of internal loop-forming (dA.dT)N domains in pBR322 DNA has been measured over a tenfold range of [Na+]. The slopes SN = dTm/d log [Na+] are linear and decrease in magnitude with decreasing loop size N, signaling a reduction in Na+ released during the transition of these domains to the coil state. Values of SN decrease linearly with increasing N-1 in accordance with the expectation of a simple model for the occurrence of a gradient of long-range electrostatic forces at helix-coil boundaries, and extrapolate almost precisely to the value of S infinity observed for (dA.dT) infinity. These results indicate (1) less counterion is released per phosphate residue from the finite loop than from the infinite-sized loop, and (2) the difference in binding is constant for each boundary formed and independent of the size of the loop within the range examined: approximately 350 base pair (bp) greater than N greater than 71 bp. The slope of the dependence of SN on N-1 indicates the region of higher charge density at the boundary extends at least 18 A into the coil and probably 40-50 A before dropping to a value characteristic of the unperturbed coil. The free energy for excess counterion binding at boundaries can be expressed by -delta G/RT = 10.47 log[Na+] + 5.234 When the loop entropy function in a statistical mechanical algorithm for the dissociation of DNA is weighted by this quantity, calculated Tm are seen to vary by only +/- 0.09 degrees C from observed.     

Conformational changes in the unique loops bordering the ATP binding cleft of skeletal muscle myosin mediate energy transduction

Myosin has three highly-conserved, unique loops [B (320-327), M (677-689), and N (127-136)] at the entrance of the ATP binding cleft, and we previously showed that the effects of actin are mediated by a conformational change in loop M [Maruta and Homma (1998) J. Biochem. 124, 528-533]. In the present study, loops M and N were photolabeled respectively with fluorescent probes Mant-8-N(3)-ADP and Mant-2-N(3)-ADP in order to study conformational changes in the loops related to energy transduction. The effect of actin on the conformation of loop N was examined by analyzing fluorescence polarization and acrylamide quenching; the results were then compared with those previously reported for loop M. In contrast to loop M, the fluorescence polarization and the value of K(sv) of the Mant-groups crosslinked to loop N were slightly affected by actin binding. To study conformational changes in loops M and N during the ATPase cycle, FRET was analyzed using TNP-ADP.BeFn and TNP-ADP. AlF(4)(-) as FRET acceptors of Mant fluorescence. The resultant estimated distances between loop M and the active site differed for the Mant-S1.TNP-ADP.BeFn and Mant-S1.TNP-ADP.AlF(4)(-) complexes, whereas the distances between loop N and the active site differed slightly. These findings indicate that the conformation of loop M changes during the ATPase cycle, suggesting that Loop M acts as a signal transducer mediating communication between the ATP- and actin-binding sites. Loop N, by contrast, is not significantly flexible.     

Reversible unfolding of FtsZ cell division proteins from archaea and bacteria. Comparison with eukaryotic tubulin folding and assembly

The stability, refolding, and assembly properties of FtsZ cell division proteins from Methanococcus jannaschii and Escherichia coli have been investigated. Their guanidinium chloride unfolding has been studied by circular dichroism spectroscopy. FtsZ from E. coli and tubulin released the bound guanine nucleotide, coinciding with an initial unfolding stage at low denaturant concentrations, followed by unfolding of the apoprotein. FtsZ from M. jannaschii released its nucleotide without any detectable secondary structural change. It unfolded in an apparently two-state transition at larger denaturant concentrations. Isolated FtsZ polypeptide chains were capable of spontaneous refolding and GTP-dependent assembly. The homologous eukaryotic tubulin monomers misfold in solution, but fold within the cytosolic chaperonin CCT. Analysis of the extensive tubulin loop insertions in the FtsZ/tubulin common core and of the intermolecular contacts in model microtubules and tubulin-CCT complexes shows a loop insertion present at every element of lateral protofilament contact and at every contact of tubulin with CCT (except at loop T7). The polymers formed by purified FtsZ have a distinct limited protofilament association in comparison with microtubules. We propose that the loop insertions of tubulin and its CCT-assisted folding coevolved with the lateral association interfaces responsible for extended two-dimensional polymerization into microtubule polymers.