Intravital research on hydrophobic interactions in protein fibrils using a fluorescence polarization method

Fluorescent probe of acridine orange (AO) is known to be bound exclusively by materials of thick protofibril muscle fibres. The dependence of fluorescence anisotropy of AO in frog muscle fibres on the temperature has been studied. It has been found that the fluorophore orientation decreases with temperature, i.e. here the adsorbent cold denaturation takes place. This phenomenon was demonstrated for living, skinned and glycerinated muscle fibres. It shows that hydrophobic interactions contribute much to stabilization of the myosin structure. After contraction of glycerinated muscle fibres at the action of ATP, the AO fluorescence anisotropy grows independently of the temperature which is indicative of structural rearrangements in materials of thick protofibrils upon contraction.     

Interaction of bilirubin with reconstituted collagen fibrils.

1. Interaction of bilirubin with collagen fibrils was explored in a two-phase system where collagen was present as an opaque rigid gel composed of striated fibrils, and bilirubin as an aqueous solution. 2. The Ka value of the binding of bilirubin to collagen fibrils is 5.4 X 10(3)M-1. The interaction of bilirubin with collagen fibrils depends on temperature. Below 5 degrees C, the binding is greatly diminished and denaturation of collagen fibril aggregates at 52--53 degrees C into a dissolution state abolishes binding of bilirubin. 3. Salicylate and sulphanilamide do not affect the binding of bilirubin to reconstituted collagen fibrils. 4. Serum albumin (40--80mM), known to reverse the binding of bilirubin to lipids, dissociates only 50% of the bilirubin bound to collagen fibrils. This suggests that sites located on collagen participate in some tight binding of bilirubin and the corresponding binding sites on albumin do not compete with them. 5. Urea (4M) abolishes more than 70% of the binding of bilirubin to collagen. Urea and thermal denaturation studies indicate the importance of conformation and organization of collagen fibrillar aggregates for the binding of bilirubin.     

Formation of collagen type I fibrils in vitro

The assembly of collagen fibrils as a function of temperature and collagen concentration was studied. It was shown that temperature increases from 25 to 35 degrees C, the degree of ordering of collagen fibrils increases 1.5-fold at collagen concentration above 1 mg/ml and 2-fold at low collagen concentration. A maximum ordering of fibril structure occurs under conditions close to physiological (T approximately 35 degrees C and collagen concentration 1.2 mg/ml). As temperature is elevated from 30 to 35 degrees C, the packing of collagen molecules in fibrils becomes more ordered: the values of enthalpy and entropy of the transition of fibrils from the native to a disordered state decrease at all collagen concentrations used. At high collagen concentration, the dimensions of cooperative blocks in fibrils formed at 25 and 30 degrees C coincide with those of cooperative blocks of monomeric collagen in solution. Upon increasing the temperature to 35 degrees C, the dimensions of cooperative blocks increase.     

Chemical dissection and reassembly of amyloid fibrils formed by a peptide fragment of transthyretin

We have examined the chemical dissection and subsequent reassembly of fibrils formed by a ten-residue peptide to probe the forces that drive the formation of amyloid. The peptide, TTR(10-19), encompasses the A strand of the inner beta-sheet structure that lines the thyroid hormone binding site of the human plasma protein transthyretin. When dissolved in water under low pH conditions the peptide readily forms amyloid fibrils. Electron microscopy of these fibrils indicates the presence of long (>1000 nm) rigid structures of uniform diameter (approximately 14 nm). Addition of urea (3 M) to preformed fibrils disrupts these rigid structures. The partially disrupted fibrils form flexible ribbon-like arrays, which are composed of a number of clearly visible protofilaments (3-4 nm diameter). These protofilaments are highly stable, and resist denaturation in 6 M urea at 75 degrees C over a period of hours. High concentrations (>50%, v/v) of 2,2,2-trifluoroethanol also dissociate TTR(10-19) fibrils to the constituent protofilaments, but these slowly dissociate to monomeric, soluble peptides with extensive alpha-helical structure. Dilution of the denaturant or co-solvent at the stage when dissociation to protofilaments has occurred results in the efficient reassembly of fibrils. These results indicate that assembly of fibrils from protofilaments involves relatively weak and predominantly hydrophobic interactions, whereas assembly of peptides into protofilaments involves both electrostatic and hydrophobic forces, resulting in a highly stable and compact structures.     

Cellular remodelling of individual collagen fibrils visualized by time-lapse AFM

The extracellular matrix in tissues such as bone, tendon and cornea contains ordered, parallel arrays of collagen type I fibrils. Cells embedded in these matrices frequently co-align with the collagen fibrils, suggesting that ordered fibrils provide structural or signalling cues for cell polarization. To study mechanisms of matrix-induced cell alignment, we used nanoscopically defined two-dimensional matrices assembled of highly aligned collagen type I fibrils. On these matrices, different cell lines expressing integrin alpha(2)beta(1) polarized strongly in the fibril direction. In contrast, alpha(2)beta(1)-deficient cells adhered but polarized less well, suggesting a role of integrin alpha(2)beta(1) in the alignment process. Time-lapse atomic force microscopy (AFM) demonstrated that during alignment cells deform the matrix by reorienting individual collagen fibrils. Cells deformed the collagen matrix asymmetrically, revealing an anisotropy in matrix rigidity. When matrix rigidity was rendered uniform by chemical cross-linking or when the matrix was formed from collagen fibrils of reduced tensile strength, cell polarization was prevented. This suggested that both the high tensile strength and pliability of collagen fibrils contribute to the anisotropic rigidity of the matrix, leading to directional cellular traction and cell polarization. During alignment, cellular protrusions contacted the collagen matrix from below and above. This complex entanglement of cellular protrusions and collagen fibrils may further promote cell alignment by maximizing cellular traction.     

Mechanical properties of collagen fibrils

The formation of collagen fibers from staggered subfibrils still lacks a universally accepted model. Determining the mechanical properties of single collagen fibrils (diameter 50-200 nm) provides new insights into collagen structure. In this work, the reduced modulus of collagen was measured by nanoindentation using atomic force microscopy. For individual type 1 collagen fibrils from rat tail, the modulus was found to be in the range from 5 GPa to 11.5 GPa (in air and at room temperature). The hypothesis that collagen anisotropy is due to the subfibrils being aligned along the fibril axis is supported by nonuniform surface imprints performed by high load nanoindentation.     

Hexafluoroisopropanol induces amyloid fibrils of islet amyloid polypeptide by enhancing both hydrophobic and electrostatic interactions

Although amyloid fibrils deposit with various proteins, the comprehensive mechanism by which they form remains unclear. We studied the formation of fibrils of human islet amyloid polypeptide associated with type II diabetes in the presence of various concentrations of 1,1,1,3,3,3-hexafluoroisopropanol (HFIP) under acidic and neutral pH conditions using CD, amyloid-specific thioflavin T fluorescence, fluorescence imaging with thioflavin T, and atomic force microscopy. At low pH, the formation of fibrils was promoted by HFIP with an optimum at 5% (v/v). At neutral pH in the absence of HFIP, significant amounts of amorphous aggregates formed in addition to the fibrils. The addition of HFIP suppressed the formation of amorphous aggregates, leading to a predominance of fibrils with an optimum effect at 25% (v/v). Under both conditions, higher concentrations of HFIP dissolved the fibrils and stabilized the α-helical structure. The results indicate that fibrils and amorphous aggregates are different types of precipitates formed by exclusion from water-HFIP mixtures. The exclusion occurs through the combined effects of hydrophobic interactions and electrostatic interactions, both of which are strengthened by low concentrations of HFIP, and a subtle balance between the two types of interactions determines whether the fibrils or amorphous aggregates dominate. We suggest a general view of how the structure of precipitates varies dramatically from single crystals to amyloid fibrils and amorphous aggregates.     

Structure and orientation of peptide inhibitors bound to beta-amyloid fibrils

Polymerization of the soluble beta-amyloid peptide into highly ordered fibrils is hypothesized to be a causative event in the development of Alzheimer's disease. Understanding the interactions of Abeta with inhibitors on an atomic level is fundamental for the development of diagnostics and therapeutic approaches, and can provide, in addition, important indirect information of the amyloid fibril structure. We have shown recently that trRDCs can be measured in solution state NMR for peptide ligands binding weakly to amyloid fibrils. We present here the structures for two inhibitor peptides, LPFFD and DPFFL, and their structural models bound to fibrillar Abeta(14-23) and Abeta(1-40) based on transferred nuclear Overhauser effect (trNOE) and transferred residual dipolar coupling (trRDC) data. In a first step, the inhibitor peptide structure is calculated on the basis of trNOE data; the trRDC data are then validated on the basis of the trNOE-derived structure using the program PALES. The orientation of the peptide inhibitors with respect to Abeta fibrils is obtained from trRDC data, assuming that Abeta fibrils orient such that the fibril axis is aligned in parallel with the magnetic field. The trRDC-derived alignment tensor of the peptide ligand is then used as a restraint for molecular dynamics docking studies. We find that the structure with the lowest rmsd value is in agreement with a model in which the inhibitor peptide binds to the long side of an amyloid fibril. Especially, we detect interactions involving the hydrophobic core, residues K16 and E22/D23 of the Abeta sequence. Structural differences are observed for binding of the inhibitor peptide to Abeta14-23 and Abeta1-40 fibrils, respectively, indicating different fibril structure. We expect this approach to be useful in the rational design of amyloid ligands with improved binding characteristics.     

The role of extrahelical peptides in stabilization of collagen fibrils

A quantitative model for fibril assembly of type I collagen was extended to include the explicit effect of extrahelical peptides. The collagen molecule was simulated by rod-like sequences to which short, rigid tails were connected by "nondimensional" flexible joints. Three collagen structures were studied: (1) intact collagen, simulated by a rod of axial ratio 200 (The axial ratio x was taken as a segment length) with two tails of length x = 1 and x = 2, respectively, appended to each end; (2) pepsin-digested collagen, simulated by one rigid segment of length 200 and one tail of length 1; and (3) pronase-digested collagen, by a single rigid segment of length x = 200. Phase equilibria of such structures were calculated, using a lattice theory of Matheson and Flory, and the relation of the polymer-solvent interaction parameter chi to the equilibrium solubility was determined. The chi for each collagen species was then related to temperature (T) and ionic strength (I), based on the approximation that local (per segment) stabilization of collagen fibrils was due to hydrophobic and electrostatic forces only. Solubility vs temperature curves for all three collagen species were computed and compared to published experimental data. From the chi factors for each species, the composite chi was resolved into components representing energetic contributions of the extrahelical peptides relative to the helix, which were interpreted in terms of hydrophobic or electrostatic interactions stabilizing the collagen fibril.     

Probing the pressure-temperature stability of amyloid fibrils provides new insights into their molecular properties

A number of medical disorders, including Alzheimer's disease and type II diabetes, is characterised by the deposition of amyloid fibrils in tissue. The insolubility and size of the fibrils has largely precluded the determination of their structures at high resolution. Studies probing the stability of amyloid fibrils can reveal which non-covalent interactions are important in the formation and maintenance of the fibril structure. In particular, we review here the use of high hydrostatic pressure and high temperature as perturbation techniques. In general, small aggregates formed early in the assembly process can be dissociated by high pressure, but mature amyloid fibrils are highly pressure stable. This finding suggests that a temporal transition occurs during which side chain packing and hydrogen bond formation are optimised, whereas the hydrophobic effect and electrostatic interactions play a dominant role in the early stages of the aggregation. High temperatures, however, can disrupt most aggregates. Though the observed stability of amyloid fibrils is not unique to these structures, the notion that amyloid fibrils can represent the global minimum in free energy is supported by this type of investigations. Some implications regarding the nature of toxic species, associated with at least many of the amyloid disorders, and recently proposed structural models are discussed.     

Diffusional anisotropy in collagenous tissues: fluorescence imaging of continuous point photobleaching

Molecular transport in avascular collagenous tissues such as articular cartilage occurs primarily via diffusion. The presence of ordered structures in the extracellular matrix may influence the local transport of macromolecules, leading to anisotropic diffusion depending on the relative size of the molecule and that of extracellular matrix structures. Here we present what we believe is a novel photobleaching technique for measuring the anisotropic diffusivity of macromolecules in collagenous tissues. We hypothesized that macromolecular diffusion is anisotropic in collagenous tissues, depending on molecular size and the local organization of the collagen structure. A theoretical model and experimental protocol for fluorescence imaging of continuous point photobleaching was developed to measure diffusional anisotropy. Significant anisotropy was observed in highly ordered collagenous tissues such as ligament, with diffusivity ratios >2 along the fiber direction compared to the perpendicular direction. In less-ordered tissues such as articular cartilage, diffusional anisotropy was dependent on site in the tissue and size of the diffusing molecule. Anisotropic diffusion was also dependent on the size of the diffusing molecule, with greatest anisotropy observed for larger molecules. These findings suggest that diffusional transport of macromolecules is anisotropic in collagenous tissues, with higher rates of diffusion along primary orientation of collagen fibers.     

Formation of amyloid fibrils by peptides derived from the bacterial cold shock protein CspB.

Three peptides covering the sequence regions corresponding to the first two (CspB-1), the first three (CspB-2), and the last two (CspB-3) beta-strands of CspB, the major cold shock protein of Bacillus subtilis, have been synthesized and analyzed for their conformations in solution and for their precipitation behavior. The peptides are nearly insoluble in water, but highly soluble in aqueous solutions containing 50% acetonitrile (pH 4.0). Upon shifts of the solvent condition toward lower or higher acetonitrile concentrations, the peptides all form fibrils resembling those observed in amyloid associated diseases. These fibrils have been identified and characterized by electron microscopy, binding of the dye congo red, and X-ray fiber diffraction. Characterization of the peptides in solution by circular dichroism and NMR spectroscopy shows that the formation of these fibrils does not require specific preformed secondary structure in the solution state species. While the majority of the soluble fraction of each peptide is monomeric and unstructured, different types of structures including alpha-helical, beta-sheet, and random coil conformations are observed under conditions that eventually lead to fibril formation. We conclude that the absence of tertiary contacts under solution conditions where binding interactions between peptide units are still favorable is a crucial requirement for amyloid formation. Thus, fragmentation of a sequence, like partial chemical denaturation or mutation, can enhance the capacity of specific protein sequences to form such fibrils.     

Discrete integration of collagen XVI into tissue-specific collagen fibrils or beaded microfibrils.

The structural and functional diversity of extracellular matrices is determined, not only by individual macromolecules, but even more decisively, by the alloyed aggregates they form. Although quantitatively major matrix molecules can occur ubiquitously, their organization varies from one tissue to another due to their amalgamation with specific sets of minor components. Here, we show that the fibril-associated collagen with interrupted triple helices collagen XVI is unique in that, depending on the tissue context, it can be incorporated into distinct suprastructural aggregates. In papillary dermis, the protein unexpectedly does not occur in banded collagen fibrils, but rather, is a component of specialized fibrillin-1-containing microfibrils. In territorial cartilage matrix, however, collagen XVI is not a component of aggregates containing fibrillin-1. Instead, the protein resides in a discrete population of thin, weakly banded collagen fibrils also containing collagens II and XI. Collagen IX also occurs in this population of fibrils, but at longitudinal locations discrete from those of collagen XVI. This suprastructural versatility of a collagen is without precedent and highlights pivotal differences in the tissue-specific organization of matrix aggregate structures.     

Characterization of the Heterogeneity and Specificity of Interpolypeptide Interactions in Amyloid Protofibrils by Measurement of Site-Specific Fluorescence Anisotropy Decay Kinetics

The aggregation of proteins often results in highly ordered fibrillar structures. While significant insights have been obtained on structural aspects of amyloid fibrils, little is known about the structures of protofibrils, which are presumed to be the precursors of fibrils. An understanding of the molecular mechanism of the formation of protofibrils and fibrils requires information on the landscape of interpeptide interactions. This work addresses this question by using, as a model protein, barstar, which forms protofibrils and fibrils at low (< 3) pH. Use was made of the heterogeneity of aggregate populations encountered during fibril formation. Population heterogeneity was scored through rotational dynamics monitored by time-resolved fluorescence anisotropy of an environment-sensitive fluorophore, 5-((((2-iodoacetyl)amino)ethyl)amino)naphthalene-1-sulfonic acid (1,5-IAEDANS), attached to specific locations in the protein. Firstly, it was observed that barstar, when labeled at certain locations with 1,5-IAEDANS, did not form mixed protofibrils with the corresponding unlabeled protein. Labeled and unlabeled proteins formed protofibrils as separate populations. A two-population model of fluorescence anisotropy decay kinetics exhibiting a ‘dip-and-rise’ behavior was the main readout in arriving at this conclusion. Additional support for this conclusion came from the fluorescence lifetime of the probe 1,5-IAEDANS. Subsequently, the location of the fluorophore was moved along the length of the protein in nine mutant proteins, and the capability to form mixed fibrils was assessed. The results revealed that about two-thirds of the protein sequence at the C-terminal end of the protein was intimately involved in the formation of ordered protofibrils, probably forming the core, while the remaining one-third of the protein (i.e., the N-terminal region) remained largely noninteractive and flexible. This methodology can be used as a general strategy to identify regions of a given protein sequence involved in interprotein interactions in amyloid protofibrils.     

Time-dependent increase in the stability of collagen fibrils formed in vitro. I. Effects of pH and salt concentration on the dissolution of the fibrils.

The time-dependent increase in stability, as measured in terms of the rate of dissolution, of collagen fibrils formed in vitro from pepsin-treated collagen was significantly affected only by temperature, and not by either ionic strength or pH. This is in contrast with collagen fibril formation, a process which is greatly affected by ionic strength and pH. Within the range of temperature 29-37 degrees C, lower temperature caused slower fibril formation and faster fibril stabilization. These results suggest that the intermolecular interactions involved in stabilizing collagen fibrils are entirely different from those involved in fibril formation. Based on kinetic analysis of the dissolution and stabilization of the fibrils, it is proposed that collagen molecules first form unstable fibrils which become gradually stabilized on prolonged incubation, without necessarily introducing covalent cross-links.     

Benzo[a]pyrene-collagen interactions

In vitro interactions of benzo[a]pyrene (BaP) with acid-soluble type I collagen from rat tail tendon have been investigated. The fluorescence of BaP increases in the presence of collagen. Bound BaP inhibits the formation of collagen fibrils in solution. When BaP-collagen complexes are irradiated in air with UV (365 nm) light, BaP rapidly undergoes photooxidation with the further inhibition of fibril formation. Viscosity and circular dichroism (CD) studies show that neither BaP nor further UV-irradiation alters the size or helical conformation of the protein. During thermal denaturation of collagen, BaP fluorescence changes. Collagen from young rat tail tendon shows a pronounced drop at about 38 degrees C, whereas that from old rat tail tendon exhibits an increase with a plateau in the same temperature range. These anomalous changes are observed when tyrosine residues, present only in the non-helical terminal telopeptides of collagen, are excited at 275 nm, but not by direct BaP excitation at 387 nm. These findings suggest that the specific hydrophobic telopeptide region, which plays an important role in fibril formation, are affected by bound BaP.     

A theoretical study of polymorphism in VQIVYK fibrils

The VQIVYK fragment from the Tau protein, also known as PHF6, is essential for aggregation of Tau into neurofibrillary lesions associated with neurodegenerative diseases. VQIVYK itself forms amyloid fibrils composed of paired β-sheets. Therefore, the full Tau protein and VQIVYK fibrils have been intensively investigated. A central issue in these studies is polymorphism, the ability of a protein to fold into more than one structure. Using all-atom molecular simulations, we generate five stable polymorphs of VQIVYK fibrils, establish their relative free energy with umbrella sampling methods, and identify the side chain interactions that provide stability. The two most stable polymorphs, which have nearly equal free energy, are formed by interdigitation of the mostly hydrophobic VIY “face” sides of the β-sheets. Another stable polymorph is formed by interdigitation of the QVK “back” sides. When we turn to examine structures from cryo-electron microscopy experiments on Tau filaments taken from diseased patients or generated in vitro, we find that the pattern of side chain interactions found in the two most stable face-to-face as well as the back-to-back polymorphs are recapitulated in amyloid structures of the full protein. Thus, our studies suggest that the interactions stabilizing PHF6 fibrils explain the amyloidogenicity of the VQIVYK motif within the full Tau protein and provide justification for the use of VQIVYK fibrils as a test bed for the design of molecules that identify or inhibit amyloid structures.     

Membrane effects of lysozyme amyloid fibrils

The influence of mature lysozyme fibrils on the structural and physical properties of model membranes composed of phosphatidylcholine (PC) and its mixtures with cardiolipin (CL) (10 mol%) and cholesterol (Chol) (30 mol%) was studied using fluorescent probes DPH, pyrene, Laurdan and MBA. Analysis of pyrene fluorescence spectra along with the measurements of DPH fluorescence anisotropy revealed that the structure of hydrocarbon chains region of lipid bilayer is not affected by the fibrillar aggregates of lysozyme. In contrast, probing the membrane effects by Laurdan and MBA showed the rise of both the generalized polarization of Laurdan and the MBA fluorescence anisotropy, suggesting that amyloid protein induces reduction of bilayer hydration and increase of lipid packing in the interfacial region of model membranes.     

Stress-strain experiments on individual collagen fibrils

Collagen, a molecule consisting of three braided protein helices, is the primary building block of many biological tissues including bone, tendon, cartilage, and skin. Staggered arrays of collagen molecules form fibrils, which arrange into higher-ordered structures such as fibers and fascicles. Because collagen plays a crucial role in determining the mechanical properties of these tissues, significant theoretical research is directed toward developing models of the stiffness, strength, and toughness of collagen molecules and fibrils. Experimental data to guide the development of these models, however, are sparse and limited to small strain response. Using a microelectromechanical systems platform to test partially hydrated collagen fibrils under uniaxial tension, we obtained quantitative, reproducible mechanical measurements of the stress-strain curve of type I collagen fibrils, with diameters ranging from 150-470 nm. The fibrils showed a small strain (epsilon < 0.09) modulus of 0.86 +/- 0.45 GPa. Fibrils tested to strains as high as 100% demonstrated strain softening (sigma(yield) = 0.22 +/- 0.14 GPa; epsilon(yield) = 0.21 +/- 0.13) and strain hardening, time-dependent recoverable residual strain, dehydration-induced embrittlement, and susceptibility to cyclic fatigue. The results suggest that the stress-strain behavior of collagen fibrils is dictated by global characteristic dimensions as well as internal structure.     

Bone structure: from angstroms to microns.

Bone has a complex hierarchical structure, which despite much investigation, is still not well understood. Here we bring together pieces of this complicated puzzle, albeit from different sources, to present a tentative overview of bone structure. The basic building blocks are the extremely small plate-shaped crystals of carbonate apatite, just hundreds of angstroms long and wide and some 20-30 A thick. They are arranged in parallel layers within the collagenous framework. At the next hierarchical level these mineral-filled collagen fibrils are ordered into arrays in which the fibril axes and the crystal layers are all organized into a 3-dimensional structure that makes up a single layer or lamella of bone a few microns thick. The orientations of the collagen fibrils and the crystal layers in alternating lamellae of rat bone differ such that in the thinner lamellae, the fibrils and the crystal layers are parallel to the lamellar boundaries. In the thicker lamellae the fibrils are parallel to the boundary, but the crystal layers are rotated out of the plane of the boundary. In many bones these alternating lamellae are organized into even larger ordered structures to produce what is truly a remarkably ordered material, all the way from the molecular scale to the macroscopic product.