NMR identification and characterization of the flexible regions in the 160 kDa molten globule-like aggregate of barstar at low pH

Intrinsically disordered proteins: modes of binding with emphasis on disordered domains

Our notions of protein function have long been determined by the protein structure-function paradigm. However, the idea that protein function is dictated by a prerequisite complementarity of shapes at the binding interface is becoming increasingly challenged. Interactions involving intrinsically disordered proteins (IDPs) have indicated a significant degree of disorder present in the bound state, ranging from static disorder to complete disorder, termed 'random fuzziness'. This review assesses the anatomy of an IDP and relates how its intrinsic properties permit promiscuity and allow for the various modes of interaction. Furthermore, a mechanistic overview of the types of disordered domains is detailed, while also relating to a recent example and the kinetic and thermodynamic principles governing its formation.

Distinct β-sheet structure in protein aggregates determined by ATR-FTIR spectroscopy

Attenuated total reflectance Fourier transform infrared spectroscopy (ATR-FTIR) was used to study the conformation of aggregated proteins in vivo and in vitro. Several different protein aggregates, including amyloid fibrils from several peptides and polypeptides, inclusion bodies, folding aggregates, soluble oligomers, and protein extracts from stressed cells, were examined in this study. All protein aggregates demonstrate a characteristic new β structure with lower-frequency band positions. All protein aggregates acquire this new β band following the aggregation process involving intermolecular interactions. The β sheets in some proteins arise from regions of the polypeptide that are helical or non β in the native conformation. For a given protein, all types of the aggregates (e.g., inclusion bodies, folding aggregates, and thermal aggregates) showed similar spectra, indicating that they arose from a common partially folded species. All of the aggregates have some nativelike secondary structure and nonperiodic structure as well as the specific new β structure. The new β could be most likely attributed to stronger hydrogen bonds in the intermolecular β-sheet structure present in the protein aggregates.

Solvent-induced tuning of internal structure in a protein amyloid protofibril

An important goal in studies of protein aggregation is to obtain an understanding of the structural diversity that is characteristic of amyloid fibril and protofibril structures at the molecular level. In this study, what to our knowledge are novel assays based on time-resolved fluorescence anisotropy decay and dynamic quenching measurements of a fluorophore placed at different specific locations in the primary structure of a small protein, barstar, have been used to determine the extent to which the protein sequence participates in the structural core of protofibrils. The fluorescence measurements reveal the structural basis of how modulating solvent polarity results in the tuning of the protofibril conformation from a pair of parallel β-sheets in heat-induced protofibrils to a single parallel β-sheet in trifluorethanol-induced protofibrils. In trifluorethanol-induced protofibrils, the single β-sheet is shown to be built up from in-register β-strands formed by nearly the entire protein sequence, while in heat-induced protofibrils, the pair of β-sheets motif is built up from β-strands formed by only the last two-third of the protein sequence.

High-resolution conformation and backbone dynamics of a soluble aggregate of apomyoglobin119

The structure and dynamics of soluble misfolded aggregates are poorly understood, despite their importance in protein science and disease. Water-soluble self-associated species that do not become insoluble over time are invaluable tools for high-resolution conformational studies aimed at dissecting the determinants of self-association. Here, we characterize the soluble model aggregate apomyoglobin(119) (apoMb(119)), generated upon truncating the residues corresponding to the C-terminal helix of sperm whale apomyoglobin. The secondary structure and backbone dynamics of apoMb(119), determined by multidimensional NMR at pH 6.0, reveal the presence of an N-terminal slow-tumbling core and a highly disordered flexible C-terminus displaying residual helicity and large-amplitude backbone motions on the picosecond-to-nanosecond timescale. The backbone of the apoMb(119) aggregate assumes progressively increased mobility as residues get further removed from the nonpolar core and closer to the more hydrophilic C-terminal end. This structural motif establishes a useful paradigm for the topology of soluble misfolded protein aggregates in aqueous solution in the absence of stabilizing additives. The partially helical and flexible C-terminus of apoMb(119)'s aggregate is in interesting contrast with the amyloid-related globulomers, which display dangling ends rich in β-strand. Finally, we investigate how a molecular chaperone, the substrate-binding domain of DnaK, interferes with apoMb(119)'s aggregation.

Fluoroalcohol-induced modulation of the pathway of amyloid protofibril formation by barstar

To understand how the conformational heterogeneity of protofibrils formed by any protein, as well as the mechanisms of their formation, are modulated by a change in aggregation conditions, we studied the formation of amyloid protofibrils by barstar at low pH by multiple structural probes in the presence of hexafluoroisopropanol (HFIP). In the presence of 10% HFIP, aggregation proceeds with the transient formation of spherical oligomers and leads to the formation of both protofibrils and fibrils. Curly short protofibrils and fibrils are seen to form early during the aggregation reaction, and both are seen to grow gradually in length during the course of the reaction. Atomic force microscopy images reveal that the HFIP-induced protofibrils are long (∼300 nm in length), curly, and beaded and appear to be composed primarily of β-sheet bilayers, with heights of ∼2.4 nm. The protofibrils formed in the presence of HFIP differ in both their structures and their stabilities from the protofibrils formed either in the absence of alcohol or in the presence of a related alcohol, trifluoroethanol (TFE). Aggregation appears to proceed via an isodesmic polymerization mechanism. Internal structure in the growing aggregates changes in two stages during protofibril formation. In the first stage, an α-helix-rich oligomeric intermediate is formed. In the second stage, the level of β-sheet structure increases at the expense of some α-helical structure. The second stage itself appears to occur in two distinct steps. The creation of thioflavin T binding sites occurs concomitantly with aggregate elongation and is seen to precede the change in secondary structure. The long straight fibrils with characteristic heights of 8-10 nm, which form in the course of the HFIP-induced aggregation reaction, have not been observed to form either in the absence of alcohol or in the presence of TFE.

On the stability of the soluble amyloid aggregates

Many amyloid proteins form metastable soluble aggregates (or protofibrils, or protein nanoparticles, with characteristic sizes from approximately 10 to a few hundred nm). These can coexist with protein monomers and amyloid precipitates. These soluble aggregates are key determinants of the toxicity of these proteins. It is therefore imperative to understand the physical basis underlying their stability. Simple nucleation theory, typically applied to explain the kinetics of amyloid precipitation, fails to predict such intermediate stable states. We examine stable nanoparticles formed by the Alzheimer's amyloid-beta peptide (40 and 42 residues), and by the protein barstar. These molecules have different hydrophobicities, and therefore have different short-range attractive interactions between the molecules. We also vary the pH and the ionic strength of the solution to tune the long-range electrostatic repulsion between them. In all the cases, we find that increased long-range repulsion results in smaller stable nanoparticles, whereas increased hydrophobicity produces the opposite result. Our results agree with a charged-colloid type of model for these particles, which asserts that growth-arrested colloid particles can result from a competition between short-range attraction and long-range repulsion. The nanoparticle size varies superlinearly with the ionic strength, possibly indicating a transition from an isotropic to a linear mode of growth. Our results provide a framework for understanding the stability and growth of toxic amyloid nanoparticles, and provide cues for designing effective destabilizing agents.

Structurally distinct amyloid protofibrils form on separate pathways of aggregation of a small protein

Understanding the structural as well as mechanistic basis of the conformational polymorphism evident during amyloid protofibril and fibril formation by proteins is an important goal in the study of protein aggregation. In this report, we compare two separate routes to amyloid protofibril formation by the small protein barstar, one induced by the addition of trifluoroethanol (TFE) and the other by heat. The study reveals that the TFE-induced aggregation of barstar leads to protofibrils that differ from heat-induced protofibrils in their external dimensions and internal structures as well as in the mechanisms of their formation. Atomic force microscopy reveals that the TFE-induced protofibrils have about half the thickness of the heat-induced protofibrils. The thickness of the TFE-induced protofibrils (1.14 +/- 0.24) suggests that they form a beta-sheet monolayer, while the thickness of the heat-induced protofibrils (2.56 +/- 0.32) suggests that they are built up from a pair (bilayer) of beta-sheets. Fourier-transform infrared (FTIR) as well as circular dichroism (CD) spectroscopy shows that the heat-induced protofibrils are not pure beta-sheet structures but that they also contain other structures (alpha-helix and/or random coil). In contrast, the TFE-induced protofibrils contain more beta-sheet structures and less of other structures, if any. The FTIR and CD spectra also reveal that the two differently created protofibrils differ in the internal structures of their beta-sheets. The TFE-induced protofibrils differ from the heat-induced protofibrils also in the kinetics of their formation. For the heat-induced reaction, the kinetics are monophasic without any lag phase, while the kinetics of the formation of TFE-induced protofibrils are sigmoidal with an initial lag phase. It appears that the TFE-induced and the heat-induced reactions involve distinct pathways for the formation of amyloid protofibrils. The existence of alternative pathways leading to amyloid protofibrils of distinct structures has important implications in understanding the kinetic origin of amyloid polymorphism.

Conformational conversion may precede or follow aggregate elongation on alternative pathways of amyloid protofibril formation

A major goal in the study of protein aggregation is to understand how the conformational heterogeneity characteristic of the process leads to structurally distinct amyloid fibrils. The small protein barstar is known to form amyloid protofibrils in multiple steps at low pH: a small oligomer, the A-form, first transforms into a larger spherical higher oligomeric intermediate (HOI), which then self-associates to form the elongated protofibril. To determine how the conformational conversion reaction during aggregation is coupled to the process of protofibril formation, cysteine-scanning mutagenesis was first used to identify specific residue positions in the protein sequence, which are important in defining the nature of the aggregation process. Two classes of mutant proteins, which are distinguished by their kinetics of aggregation at high protein concentration, have been identified: Class I mutant proteins undergo conformational conversion, as measured by an increase in thioflavin T binding ability and an increase in circular dichroism at 216 nm, significantly faster than Class II mutant proteins. At low protein concentration, the rates of conformational conversion are, however, identical for both classes of mutant proteins. At high protein concentration, the two classes of mutant proteins can be further distinguished on the basis of their rates of protofibril growth, as determined from dynamic light-scattering measurements. For Class I mutant proteins, protofibril elongation occurs at the same, or slightly faster, rate than conformational conversion. For Class II mutant proteins, protofibril elongation is significantly slower than conformational conversion. Dynamic light scattering measurements and atomic force microscopy imaging indicate that for the Class I mutant proteins, conformational conversion occurs concurrently with the self-association of prefibrillar HOIs into protofibrils. On the other hand, for the Class II mutant proteins, the prefibrillar HOI first undergoes conformational conversion, and the conformationally converted HOIs then self-associate to form protofibrils. The two classes of mutant proteins appear, therefore, to use structurally distinct pathways to form amyloid protofibrils. On one pathway, conformational conversion occurs along with, or after, elongation of the oligomers; on the other pathway, conformational conversion precedes elongation of the oligomers. Single mutations in the protein can cause aggregation to switch from one pathway to the other. Importantly, the protofibrils formed by the two classes of mutant proteins have significantly different diameters and different internal structures.

13C NMR characterization of an exchange reaction between CO and CO2 catalyzed by carbon monoxide dehydrogenase

Carbon monoxide dehydrogenase (CODH) catalyzes the reversible oxidation of CO to CO2 at a nickel-iron-sulfur cluster (the C-cluster). CO oxidation follows a ping-pong mechanism involving two-electron reduction of the C-cluster followed by electron transfer through an internal electron transfer chain to external electron acceptors. We describe 13C NMR studies demonstrating a CODH-catalyzed steady-state exchange reaction between CO and CO2 in the absence of external electron acceptors. This reaction is characterized by a CODH-dependent broadening of the 13CO NMR resonance; however, the chemical shift of the 13CO resonance is unchanged, indicating that the broadening is in the slow exchange limit of the NMR experiment. The 13CO line broadening occurs with a rate constant (1080 s-1 at 20 degrees C) that is approximately equal to that of CO oxidation. It is concluded that the observed exchange reaction is between 13CO and CODH-bound 13CO2 because 13CO line broadening is pH-independent (unlike steady-state CO oxidation), because it requires a functional C-cluster (but not a functional B-cluster) and because the 13CO2 line width does not broaden. Furthermore, a steady-state isotopic exchange reaction between 12CO and 13CO2 in solution was shown to occur at the same rate as that of CO2 reduction, which is approximately 750-fold slower than the rate of 13CO exchange broadening. The interaction between CODH and the inhibitor cyanide (CN-) was also probed by 13C NMR. A functional C-cluster is not required for 13CN- broadening (unlike for 13CO), and its exchange rate constant is 30-fold faster than that for 13CO. The combined results indicate that the 13CO exchange includes migration of CO to the C-cluster, and CO oxidation to CO2, but not release of CO2 or protons into the solvent. They also provide strong evidence of a CO2 binding site and of an internal proton transfer network in CODH. 13CN- exchange appears to monitor only movement of CN- between solution and its binding to and release from CODH.

Mechanism of Formation of Amyloid Protofibrils of Barstar from Soluble Oligomers: Evidence for Multiple Steps and Lateral Association Coupled to Conformational Conversion

Understanding the heterogeneity of the soluble oligomers and protofibrillar structures that form initially during the process of amyloid fibril formation is a critical aspect of elucidating the mechanism of amyloid fibril formation by proteins. The small protein barstar offers itself as a good model protein for understanding this aspect of amyloid fibril formation, because it forms a stable soluble oligomer, the A form, at low pH, which can transform into protofibrils. The mechanism of formation of protofibrils from soluble oligomer has been studied by multiple structural probes, including binding to the fluorescent dye thioflavin T, circular dichroism and dynamic light scattering, and at different temperatures and different protein concentrations. The kinetics of the increase in any probe signal are single exponential, and the rate measured depends on the structural probe used to monitor the reaction. Fastest is the rate of increase in the mean hydrodynamic radius, which grows from a value of 6 nm for the A form to 20 nm for the protofibril. Slower is the rate of increase in thioflavin T binding capacity, and slowest is the rate of increase in circular dichroism at 216 nm, which occurs at about the same rate as that of the increase in light scattering intensity. The dynamic light scattering measurements suggest that the A form transforms completely into larger size aggregates at an early stage during the aggregation process. It appears that structural changes within the aggregates occur at the late stages of assembly into protofibrils. For all probes, and at all temperatures, no initial lag phase in protofibril growth is observed for protein concentrations in the range of 1 microM to 50 microM. The absence of a lag phase in the increase of any probe signal suggests that aggregation of the A form to protofibrils is not nucleation dependent. In addition, the absence of a lag phase in the increase of light scattering intensity, which changes the slowest, suggests that protofibril formation occurs through more than one pathway. The rate of aggregation increases with increasing protein concentration, but saturates at high concentrations. An analysis of the dependence of the apparent rates of protofibril formation, determined by the four structural probes, indicates that the slowest step during protofibil formation is lateral association of linear aggregates. Conformational conversion occurs concurrently with lateral association, and does so in two steps leading to the creation of thioflavin T binding sites and then to an increase in beta-sheet structure. Overall, the study indicates that growth during protofibril formation occurs step-wise through progressively larger and larger aggregates, via multiple pathways, and finally through lateral association of critical aggregates.

Alanine check points in HNN and HN(C)N spectra

Rapid resonance assignment is a key requirement in structural genomics research by NMR. In this context we present here two new pulse sequences, namely, HNN-A and HN(C)N-A that have been developed by simple modification of the previously described pulse sequences, HNN and HN(C)N [S.C. Panchal, N.S. Bhavesh, R.V. Hosur, Improved 3D triple resonance experiments, HNN and HN(C)N, for H(N) and 15N sequential correlations in (13C, 15N) labeled proteins: application to unfolded proteins, J. Biomol. NMR, 20 (2001) 135-147]. These increase the number of start/check points in HNN and/or HN(C)N spectra and hence help in pacing up resonance assignment in proteins.

Probing the folding capacity and residual structures in 1-79 residues fragment of staphylococcal nuclease by biophysical and NMR methods

1-79 residues SNase fragment (SNase79) has chain length containing a sequence for helix alpha(1), omega-loop, beta(I)-sheet, and partial beta(II)-sheet of native SNase. The incomplete "beta-barrel" structural region of SNase79 makes this fragment to be interested in investigation of its conformation. For this study, we use CD, fluorescence, and NMR spectroscopy to probe the folding capacity and the residual structures in SNase79. The optical spectra obtained for SNase79 and its mutants reveal the presence of retained capacity for folding of the fragment. The NMR derived (13)C(alpha) secondary chemical shifts, (3)J(NH-Halpha) coupling constants, amide-proton temperature coefficients, interresidue NOEs, and (15)N relaxation data determine the intrinsic propensities for helix- and turn- or beta-sheet-like conformations of SNase79, which is not the result of stabilizing inter-molecular interactions by oligomerization effects. The residual turn- and helix-like structures may serve as potential local nucleation sites, whereas the residual beta(I)-sheet-like structure can be regarded as a potential non-local nucleation site in the folding of SNase79. The intrinsic local and non-local interactions in these potential initiation sites are insufficient to stabilize the folding of SNase79 due to the shortage of relevant long-range interactions from other part of the fragment. The conformational ensemble of SNase79 is a highly heterogeneous collection of interconverting conformations having transiently populated helix- and beta-sheet- or turn-like structures.

Characterization of the Formation of Amyloid Protofibrils from Barstar by Mapping Residue-specific Fluorescence Dynamics

The small protein barstar aggregates at low pH to form soluble oligomers, which can be transformed into fibrillar aggregates at an elevated temperature. To characterize structurally, with residue-specific resolution, the process of amyloid formation of barstar, as well as to monitor the increase in size that accompanies the aggregation process, time-resolved fluorescence anisotropy decay measurements have been introduced as a valuable probe. Seven different single-cysteine-containing mutant forms of barstar were made, to each of which a fluorophore was attached at the thiol group. The rotational dynamics of these seven fluorophores, as well as of the sole intrinsic tryptophan residue in the protein, were determined in the amyloid protofibrils formed, as well as in the soluble oligomers from which the protofibrils arise upon heating. Mapping of the fast rotational dynamics onto the sequence of the protein yields dynamic amplitude maps that allowed identification of the segments of the chain that possess local structure in the soluble oligomer and amyloid protofibrils. The patterns of these maps of the soluble oligomer and protofibrils are seen to be similar; and protofibrils display more local structure than do the soluble oligomers, at all residue positions studied. The observation that transformation from soluble oligomers to protofibrils does not perturb local structure significantly at eight different residue positions, suggests that the soluble oligomers transform directly into protofibrils, without undergoing drastic structural rearrangements.

Fast assignment of 15N-HSQC peaks using high-resolution 3D HNcocaNH experiments with non-uniform sampling

We describe an efficient NMR triple resonance approach for fast assignment of backbone amide resonance peaks in the 15N-HSQC spectrum. The exceptionally high resolutions achieved in the 3D HncocaNH and hNcocaNH experiments together with non-uniform sampling facilitate error-free sequential connection of backbone amides. Data required for the complete backbone amide assignment of the 56-residue protein GB1 domain were obtained in 14 h. Data analysis was vastly streamlined using a 'backbone NH walk' method to determine sequential connectivities without the need for 13C chemical shifts comparison. Amino acid residues in the sequentially connected NH chains are classified into two groups by a simple variation of the NMR pulse sequence, and the resulting 'ZeBra' stripe patterns are useful for mapping these chains to the protein sequence. In addition to resolving ambiguous assignments derived from conventional backbone experiments, this approach can be employed to rapidly assign small proteins or flexible regions in larger proteins, and to transfer assignments to mutant proteins or proteins in different ligand-binding states.

Equilibrium titrations of acid-induced unfolding–refolding and salt-induced molten globule of cytochrome c by FT-IR spectroscopy

Despite extensive investigations on the acid-unfolded and acid/salt-induced molten globule(-like) states of cytochrome c using variety of techniques, structural features of the acid-unfolded state in terms of residual secondary structures and the structural transition between the acid-unfolded and acid/salt-refolded states have not been fully characterized beyond the circular dichroism (CD) spectroscopy. It is unusual that secondary structure(s) of the unfolded state leading to the molten globule state, an important protein folding intermediate, as determined by CD was not fully corroborated by independent experimental method(s). In this study, we carried out an equilibrium titration of acid-induced unfolding and subsequent acid- and salt-induced refolding of cytochrome c using Fourier transform infrared spectroscopy. The spectral profiles of the equilibrium titration reveal new structural details about the acid-unfolded state and the structural transition associated with the acid/salt-refolded molten globule(-like) states of cytochrome c.

Native and nonnative conformational preferences in the urea-unfolded state of barstar

The refolding of barstar from its urea-unfolded state has been studied extensively using various spectroscopic probes and real-time NMR, which provide global and residue-specific information, respectively, about the folding process. Here, a preliminary structural characterization by NMR of barstar in 8 M urea has been carried out at pH 6.5 and 25 degrees C. Complete backbone resonance assignments of the urea-unfolded protein were obtained using the recently developed three-dimensional NMR techniques of HNN and HN(C)N. The conformational propensities of the polypeptide backbone in the presence of 8 M urea have been estimated by examining deviations of secondary chemical shifts from random coil values. For some residues that belong to helices in native barstar, 13C(alpha) and 13CO secondary shifts show positive deviations in the urea-unfolded state, indicating that these residues have propensities toward helical conformations. These residues are, however, juxtaposed by residues that display negative deviations indicative of propensities toward extended conformations. Thus, segments that are helical in native barstar are unlikely to preferentially populate the helical conformation in the unfolded state. Similarly, residues belonging to beta-strands 1 and 2 of native barstar do not appear to show any conformational preferences in the unfolded state. On the other hand, residues belonging to the beta-strand 3 segment show weak nonnative helical conformational preferences in the unfolded state, indicating that this segment may possess a weak preference for populating a helical conformation in the unfolded state.

Application of HN(C)N to rapid estimation of 1J(N-C(alpha)) coupling constants correlated to psi torsion angles in proteins: implication to structural genomics

We recently described a triple resonance experiment, HN(C)N, for sequential correlation of H(N) and 15N atoms in (15N, 13C) labeled proteins [J. Biomol. NMR. 20 (2001) 135]. Here, we describe an approach based on this experiment for estimation of one bond N-C(alpha) J-couplings in medium size labeled proteins, which seem to show good correlations with psi torsion angles along the protein backbone. The approach uses the ratio of the intensities of the sequential and diagonal peaks in the F(2)-F(3) planes of the HN(C)N spectrum. The reliability of the approach has been demonstrated using a short peptide wherein the coupling constants have been measured by the present method and also independently from peak splittings in HSQC spectra. The two results agree within 10%. The applicability of the procedure to proteins has been demonstrated using doubly labeled FK506 binding protein (FKBP, molecular mass approximately 12 kDa). Coupling constant estimates have been obtained for 62 out of 100 non-proline residues and they show a correlation with psi torsion angles, as has been reported before. This semi-quantitative application of HN(C)N extends the significance of the experiment especially, in the context of structural genomics, since the single experiment, not only provides a great enhancement in the speed of resonance assignment, but also provides quantitative structural information.