β-structure from the microfibillar proteins of Merino wool

The β-structure of S-caboxymethyl derivatives of microfibrillar proteins isolated from Merino wool was investigated by X-ray diffraction for comparison with the structur of β-keratin. The S-carboxymethylated microfibrillar proteins(SCMKA) w well-oriented β-films of SCMKA weer obtained by stretching the SCMKA cast films in steam up to about 300% extesnsion. It was found that the reflections in β-pattern of SCMKA may be indexed on a pseudo-orthorhombic unit cell with a =0.94 nm, b = 0.66 nm and c = nm, where the ab, and c axes are in the direction of the interchain hydrogen bonding, the main chain(fibre axis) and the side chain, respectively. The unit cell dimesnions evaluated for SCMKA were almost the same as those for β-keratin, suggeting that few peptide sequences containing S-carboxymethyl cystine may be involved in the formation of β-structure from SCMKA.     

β-structures of polypeptides with L- and D-residues

Summary It was previously shown that nuclei of-sheets surrounded by unordered segments are formed in polypeptide chains built up with alternating hydrophobic and hydrophilic residues and containing both L- and D-enantiomers. It was also established that segments of residues having the same configuration tend to segregate in these nuclei when the starting composition of stereomonomers departs from the racemic mixture.Soft acidic hydrolysis of these polymers has been studied. Kinetic measurements show two pseudo first order rate constants, in agreement with the existence of two conformational species. The unordered part of the chains is hydrolyzed more rapidly, allowing the isolation of a-fraction enriched in one enantiomer. Thus, a plausible process of enrichment in enantiomer during prebiotic evolution has been described, which however does not explain the preference of one enantiomer over the other one.     

A comparative CD study of carbonic anhydrase isoenzymes with different number of tryptophans: impact on calculation of secondary structure content.

The CD spectra of human carbonic anhydrase I and II and bovine carbonic anhydrase III were recorded and analyzed. The 3D structures of these isoenzymes are known, showing very similar secondary structure and polypeptide-chain fold. The tryptophan content, however, differs between the isoenzymes, i.e., isoenzymes I, II, and III possess 6, 7, and 8 tryptophans, respectively. All of the tryptophans except the additional tryptophans in isoenzymes II and III, i.e., W245 and W47, are conserved. Despite the fact that X-ray structure determinations showed that the isoenzymes had highly similar secondary structure, the contents of alpha-helix and beta-sheet structure differed considerably when using different CD algorithms for estimation of the fractions of various secondary structural elements. This shows that aromatic amino acids also interfere in the wavelength region (far-UV) used to calculate the amount of secondary structure. Such interference is especially problematic when analyzing proteins like carbonic anhydrase, which consist mainly of beta-structure that gives rise to weak ellipticity bands, compared to the bands arising from alpha-helical structure.     

Conformational studies on poly(N-δ-trimethyl-l-ornithine)

$\text{Poly}\text{(N-δ-}\text{trimethyl-}\text{l}\text{-ornithine}$), (Me₃Orn)_n, is usually not able to attain the α-helical conformation in aqueous solution independent of its pH value; however, it becomes α-helical at low concentrations of sodium perchlorate over a wide pH range according to the circular dichorism (c.d.) spectra. Cl^?, SO₄^2? and H₂PO₄^? do not induce α-helix formation. One can conclude that a distinct topology of the anions bound by the side chains is responsible for the α-helix-inducing effect of some water-structure-breaking anions such as perchlorate. This means that the anions are inserted between the ?N⁺ of the side groups shielding the positive charges repelling one another. The insertion of the anions requires that the water molecules surrounding the ions can be stripped off, which is easily possible if they are water-structure-breaking ones. At higher perchlorate concentrations, the c.d. spectrum changes. It is characterized by a negative shoulder near 208 nm and a pronounced minimum at ≈ 226 nm. With increasing temperature, the c.d. spectrum of the α-helix occurs. Finally the α-helix undergoes a conformational change to the random coil. The apparent transition enthalpy ΔH_vH is remarkably lower than that of the homologue (Me₃Lys)_n, obviously due to a lower cooperativity of the transition. In contrast to poly(l-ornithine), (Orn)_n, the c.d. spectrum of (Me₃Orn)_n remains almost unchanged after adding anionic surfactants such as sodium octyl sulphate (SOS) or sodium dodecyl sulphate (SDS). In organic solvents like methanol or isopropanol, in contrast to (Orn)_a and (Lys)_n, no α-helix formation occurs. However, in mixtures of these alcohols or dioxane with water, α-helix formation is induced by perchlorate, as in pure water. The thermal stability of the α-helix in these systems is increased.     

Sonication of proteins causes formation of aggregates that resemble amyloid

Despite the widespread use of sonication in medicine, industry, and research, the effects of sonication on proteins remain poorly characterized. We report that sonication of a range of structurally diverse proteins results in the formation of aggregates that have similarities to amyloid aggregates. The formation of amyloid is associated with, and has been implicated in, causing of a wide range of protein conformational disorders including Alzheimer's disease, Huntington's disease, Parkinson's disease, and prion diseases. The aggregates cause large enhancements in fluorescence of the dye thioflavin T, exhibit green-gold birefringence upon binding the dye Congo red, and cause a red-shift in the absorbance spectrum of Congo red. In addition, circular dichroism reveals that sonication-induced aggregates have high beta-content, and proteins with significant native alpha-helical structure show increased beta-structure in the aggregates. Ultrastructural analysis by electron microscopy reveals a range of morphologies for the sonication-induced aggregates, including fibrils with diameters of 5-20 nm. The addition of preformed aggregates to unsonicated protein solutions results in accelerated and enhanced formation of additional aggregates upon heating. The dye-binding and structural characteristics, as well as the ability of the sonication-induced aggregates to seed the formation of new aggregates are all similar to the properties of amyloid. These results have important implications for the use of sonication in food, biotechnological and medical applications, and for research on protein aggregation and conformational disorders.     

A Structural Model for Apolipoprotein C-II Amyloid Fibrils: Experimental Characterization and Molecular Dynamics Simulations

The self-assembly of specific proteins to form insoluble amyloid fibrils is a characteristic feature of a number of age-related and debilitating diseases. Lipid-free human apolipoprotein C-II (apoC-II) forms characteristic amyloid fibrils and is one of several apolipoproteins that accumulate in amyloid deposits located within atherosclerotic plaques. X-ray diffraction analysis of aligned apoC-II fibrils indicated a simple cross-β-structure composed of two parallel β-sheets. Examination of apoC-II fibrils using transmission electron microscopy, scanning transmission electron microscopy, and atomic force microscopy indicated that the fibrils are flat ribbons composed of one apoC-II molecule per 4.7-Å rise of the cross-β-structure. Cross-linking results using single-cysteine substitution mutants are consistent with a parallel in-register structural model for apoC-II fibrils. Fluorescence resonance energy transfer analysis of apoC-II fibrils labeled with specific fluorophores provided distance constraints for selected donor-acceptor pairs located within the fibrils. These findings were used to develop a simple ‘letter-G-like’ β-strand-loop-β-strand model for apoC-II fibrils. Fully solvated all-atom molecular dynamics (MD) simulations showed that the model contained a stable cross-β-core with a flexible connecting loop devoid of persistent secondary structure. The time course of the MD simulations revealed that charge clusters in the fibril rearrange to minimize the effects of same-charge interactions inherent in parallel in-register models. Our structural model for apoC-II fibrils suggests that apoC-II monomers fold and self-assemble to form a stable cross-β-scaffold containing relatively unstructured connecting loops.     

Amyloid character of self-assembling proteins based on adenovirus fiber shaft sequences

Fibrous proteins found in natural materials such as silk fibroins, spider silks, and viral spikes increasingly serve as a source of inspiration for the design of novel, artificial fibrous materials. The fiber protein from the adenovirus has previously served as a model for the design of artificial, self-assembling fibers. The fibrous shaft of this protein consists of 15-amino-acid sequence repeats that fold into a triple β-spiral motif in their native context. Recombinant proteins based on multimers of simplified consensus shaft repeats were previously reported to form self-assembling fibrils from which filaments could be spun. Here, we describe the structural characterization of these fibrils; X-ray fiber diffraction, Raman spectroscopy, and Congo Red binding strongly suggest an amyloid-type structure for these fibrils, with β-strands arranged perpendicular to the fibril axis. This amyloid structure is distinct from the native β-spiral fold, and similar to amyloid structures formed by short, synthetic peptides corresponding to shaft sequences. We discuss implications for the rational design of novel fibrous materials, based on crystal structure information and knowledge of folding and assembly pathways of natural fibrous proteins.     

Rate of beta-structure formation in polypeptides

An explanation is suggested for why a marginally stable beta-structure folds extremely slowly; it is predicted that even a small increase in stability drastically accelerates beta-folding. According to the theory, this folding is a first-order phase transition, and the rate-limiting step is nucleation. The rate-determining "nucleus" (transition state) is the smallest beta-sheet that is sufficiently large to provide an overall free energy reduction during subsequent folding. If the stability of the beta-structure is low, the nucleus is large and possesses a high free energy due to having a large perimeter. When the net stability of the final beta-structure increases (due to either an increase of the beta-sheet stability or a decrease in stability of the competing structures, e.g., alpha-helices), the size and energy of a nucleus decrease and the rate of folding increases exponentially. This must result in a fast folding of polypeptides enriched by beta-forming residues (e.g., protein chains). The theory is developed for intramolecular beta-structure, but it can also explain the overall features of intermolecular beta-folding; it is applicable both to antiparallel and parallel beta-sheets. The difference in folding of beta-sheets, alpha-helices, and proteins is discussed.     

Statistical analysis of the physical properties of the 20 naturally occurring amino acids

In order to describe the conformational and other physical properties of the 20 naturally occurring amino acid residues with a minimum number of parameters, several multivariate statistical analyses were applied to 188 of their physical properties and ten orthogonal properties (factors) were obtained for the 20 amino acids without losing the information contained in the original physical properties. The analysis consisted of three main steps. First, 72 of the physical properties were eliminated from further consideration because they did not pass statistical tests that they follow a normal distribution. Second, the remaining 116 physical properties of the amino acids were classified by a cluster analysis to eliminate duplications of highly correlated physical properties. This led to nine clusters, each of which was characterized by an average characteristic property, namely bulk, two hydrophobicity indices for free amino acids, one hydrophobicity index for amino acid residues in a protein, two types of -structure preference, -helix preference, and two types of bend-structure preference. The physical properties within a given cluster were highly correlated with each other, but the correlation between clusters was low. Third, a factor analysis was applied to the nine average classified properties and 16 additional physical properties to obtain a small number of orthogonal properties (ten factors). Four of these factors arise from the nine characteristic properties, and the remaining six factors were obtained from the 16 physical properties not included in the nine characteristic properties. Finally, most of the 188 physical properties could be expressed as a sum of these ten orthogonal factors, with appropriate weighting factors. Since these factors contain information relating almost all properties of all 20 amino acids, it is possible to estimate the numerical values of a property for one or two amino acids for which experimental data for this property are not available. For example, the estimated values for the Zimm-Bragg parameters at 20°C are 0.66 and 0.92 for proline and cysteine, respectively, computed from the first four factors.     

Analysis of Interactions of Buried Polar Side Chains in β-Proteins

Qualitative and quantitative analysis of polar side chains inaccessible to water molecules, as well as their interactions in 100 globular β-sheet proteins, was performed. It was shown that completely buried polar side chains are widespread in β-proteins, with their vast majority being involved in side chain-side chain or side chain-main chain interactions. An analysis of frequency of occurrence of different side chain-partner pairs demonstrated that these interactions are selective. The results were compared with similar data obtained earlier for α-helical proteins.