Biomedical subjects

Walraj S Gosal

Publications and source records attributed to Walraj S Gosal.

7 recordsLinked to original sources

PubMed2006

Amyloid under the atomic force microscope.

The atomic force microscope (AFM) is a versatile instrument that can be used to image biological samples at nanometre resolution as well as to measure inter and intra-molecular forces in air and liquid environments. This review summarises the use of AFM applied to protein and peptide self-assembly systems involved in amyloid formation. The technical principles of the AFM are outlined and its advantages and disadvantages are highlighted and discussed in the context of the rapidly developing field of amyloid research.

Amyloid beta-Peptides↗

PubMed2005

Competing pathways determine fibril morphology in the self-assembly of beta2-microglobulin into amyloid.

Despite its importance in biological phenomena, a comprehensive understanding of the mechanism of amyloid formation remains elusive. Here, we use atomic force microscopy to map the formation of beta2-microglobulin amyloid fibrils with distinct morphologies and persistence lengths, when protein concentration, pH and ionic strength are varied. Using the resulting state-diagrams, we demonstrate the existence of two distinct competitive pathways of assembly, which define an energy landscape that rationalises the sensitivity of fibril morphology on the solution conditions. Importantly, we show that semi-flexible (worm-like) fibrils, which form rapidly during assembly, are kinetically trapped species, formed via a non-nucleated pathway that is explicitly distinct from that leading to the formation of the relatively rigid long-straight fibrils classically associated with amyloid. These semi-flexible fibrils also share an antibody epitope common to other protein oligomers that are known to be toxic species linked to human disease. The results demonstrate the heterogeneity of amyloid assembly, and have important implications for our understanding of the importance of oligomeric states in amyloid disease, the origins of prion strains, and the development of therapeutic strategies.

Amyloid↗

PubMed2005

Towards an understanding of the structural molecular mechanism of beta(2)-microglobulin amyloid formation in vitro.

Deriving a complete understanding of protein self-association into amyloid fibrils across multiple distance and time scales is an enormous challenge. At small length scales, a detailed description of the partially folded protein ensemble that participates in self-assembly remains obscure. At larger length scales, amyloid fibrils are often heterogeneous, can form along multiple pathways, and are further complicated by phenomena such as phase-separation. Over the last 5 years, we have used an array of biophysical approaches in order to elucidate the structural and molecular mechanism of amyloid fibril formation, focusing on the all beta-sheet protein, beta(2)-microglubulin (beta(2)m). This protein forms amyloid deposits in the human disease 'dialysis-related amyloidosis' (DRA). We have shown that under acidic conditions beta(2)m rapidly associates in vitro to form amyloid-like fibrils that have different morphological properties, but which contain an underpinning cross-beta structure. In this review, we discuss our current knowledge of the structure of these fibrils, as well as the structural, kinetic and thermodynamic relationship between fibrils with different morphologies. The results provide some of the first insights into the shape of the self-assembly free-energy landscape for this protein and highlight the parallel nature of the assembly process. We include a detailed description of the structure and dynamics of partially folded and acid unfolded species of beta(2)m using NMR, and highlight regions thought to be important in early self-association events. Finally, we discuss briefly how knowledge of assembly mechanisms in vitro can be used to inform the design of therapeutic strategies for this, and other amyloid disorders, and we speculate on how the increasing power of biophysical approaches may lead to a fuller description of protein self-assembly into amyloid in the future.

Amyloid↗

PubMed2003

The circularization of amyloid fibrils formed by apolipoprotein C-II.

Amyloid fibrils have historically been characterized by diagnostic dye-binding assays, their fibrillar morphology, and a "cross-beta" x-ray diffraction pattern. Whereas the latter demonstrates that amyloid fibrils have a common beta-sheet core structure, they display a substantial degree of morphological variation. One striking example is the remarkable ability of human apolipoprotein C-II amyloid fibrils to circularize and form closed rings. Here we explore in detail the structure of apoC-II amyloid fibrils using electron microscopy, atomic force microscopy, and x-ray diffraction studies. Our results suggest a model for apoC-II fibrils as ribbons approximately 2.1-nm thick and 13-nm wide with a helical repeat distance of 53 nm +/- 12 nm. We propose that the ribbons are highly flexible with a persistence length of 36 nm. We use these observed biophysical properties to model the apoC-II amyloid fibrils either as wormlike chains or using a random-walk approach, and confirm that the probability of ring formation is critically dependent on the fibril flexibility. More generally, the ability of apoC-II fibrils to form rings also highlights the degree to which the common cross-beta superstructure can, as a function of the protein constituent, give rise to great variation in the physical properties of amyloid fibrils.

Amyloid↗

PubMedDate not supplied

Fibrillar beta-lactoglobulin gels: Part 1. Fibril formation and structure.

As a prelude to experimental and theoretical work on the mechanical properties of fibrillar beta-lactoglobulin gels, this paper reports the structural characterization of beta-lactoglobulin fibrils by electron and atomic force microscopy (AFM), infrared and Raman spectroscopy, and powder X-ray diffraction. Aggregates formed by incubation of beta-lactoglobulin in various alcohol-water mixtures at pH 2, and in water-trifluoroethanol (TFE) at pH 7, were found to be wormlike (approximately 7 nm in width and <500 nm in length), with a "string-of-beads" appearance. Longer (approximately 7 nm in width, and >1 microm in length), smoother, and seemingly stiffer fibrils formed on heating aqueous beta-lactoglobulin solutions at pH 2 and low ionic strength, although there was little evidence for the higher-order structures common in most amyloid-forming systems. Time-lapse AFM also revealed differences in the formation of these two fibril types: thermally induced aggregation occurring more cooperatively, in keeping with a nucleation and growth process. Only short stiff-rods (<20 nm in length) formed on heating beta-lactoglobulin at pH 7, and only complex three-dimensional "amorphous"aggregates in alcohols other than TFE at this pH. Studies of all of the pH 2 fibrils from beta-lactoglobulin, by Raman and infrared spectroscopy confirmed beta-sheet as mediating the aggregation process. Interestingly, however, some evidence for de novo helix formation for the solvent-induced systems was obtained, although it remains to be seen whether this is actually incorporated into the fibril-structure. In contrast to other amyloid systems, X-ray powder diffraction provided no evidence for extensive repeating "crystalline" structures for any of the pH 2 beta-lactoglobulin fibrils. In relation to amyloid, the lactoglobulin fibrils bear more resemblance to protofilaments than to higher-order fibril structures, these latter appearing more convincingly for thermally induced insulin fibrils (pH 2) also included in the AFM study.

Amyloid↗

PubMedDate not supplied

Fibrillar beta-lactoglobulin gels: Part 2. Dynamic mechanical characterization of heat-set systems.

Oscillatory shear rheometry (mechanical spectroscopy) has been used to study the heat-set gelation of beta-lactoglobulin at pH 2. Modulus-concentration relationships were obtained by extrapolating cure data to infinite time. In terms of theory, these fail to provide a clear distinction between the fractal description of biopolymer gels and the classical random f-functional polycondensation branching theory (cascade) approach, though the latter is preferred. Critical exponents for the sol-gel transition, derived from these data, are also discussed. Where gel time-concentration results are concerned the fractal model makes no predictions, and the cascade approach in its simplest form must be rejected in favor of a more sophisticated version involving delivery of fibrils by nucleation and growth into the random aggregation process. Over the limited concentration range accessed experimentally, cure data for the different beta-lactoglobulin solutions, reduced to the universal form G'/G'inf versus t/tgel, superimposed well for samples heated both at 80 and 75 degrees C and for different batches of protein. Studies of the frequency responses of the fully cured gels confirm the validity of the gel description given to these materials, and a study of the temperature dependence of the frequency spectrum suggests a fall in the elastic component of the modulus as temperature decreases. This contrasts with what has been found for other heat-set globular protein gels such as those from serum albumin where the gel modulus increases at lower temperatures. The present results are in good agreement with more limited amounts of pH 2 beta-lactoglobulin data published earlier, though some differences arise through a previous neglect of measurement "dead time".

Amyloid↗

PubMedDate not supplied

Fibrillar beta-lactoglobulin gels: Part 3. Dynamic mechanical characterization of solvent-induced systems.

Oscillatory shear rheometry has been used to study the gelation of beta-lactoglobulin at ambient in 50% v/v trifluoroethanol (TFE)/pH 7 aqueous buffer and in 50% v/v ethanol (EtOH)/water at pH 2. In contrast to what was found on heating aqueous solutions at pH 2 (Part 2 of this series), a more expected "chemical gelation"-like profile was found with modulus components G' and G' ' crossing over as the gels formed and then with G' ' passing through a maximum. In addition, for the EtOH system, there was a significant modulus increase at long time, suggestive of a more complex two-step aggregation scheme. Modulus-concentration relationships were obtained for both systems by extrapolating cure data to infinite time. For the TFE gels, this data was accurately described by classical branching theory, although it could also be approximated by a constant power--law relationship. Only the latter described the modulus--concentration data for the gels in ethanol, but there were problems here of greater frequency dependence of the modulus values and much less certain extrapolation. Gel times for the TFE systems showed higher power laws in the concentration than could be explained by the branching theory in its simplest form being similar, in this respect, to the heat-set systems at pH 2. Such power laws were harder to establish for the EtOH gels as for these there was evidence of gel time divergence close to a critical concentration. Reduced G'/G'inf versus t/tgel data were difficult to interpret for the gels in ethanol, but for the TFE system they were consistent with previous results for the heat-set gels and approximated master curve superposition. The frequency and temperature dependences of the final gel moduli were also studied. In general, the networks induced by alcohols appeared more flexible than those obtained by heating.

Amyloid↗