Aggregation of red blood cells studied by ultrasound backscattering

The erythrocyte aggregation phenomenon is an important factor in capillary circulation. This phenomenon can be evaluated by a number of methods (microscopic observations, viscometry, light measurements) which cannot be applied simply to in vivo measurements. In contrast, ultrasound which propagates through soft tissues allows measurement of the mechanical properties of red blood cell (RBC) suspensions which depend on the aggregation phenomenon. We devised an apparatus in order to measure in vitro the ultrasonic backscattering intensity of RBC suspensions. First, with latex particles of different sizes, the ultrasonic backscattering coefficient has been measured in order to evaluate the apparatus response. Then, the ultrasonic backscattering coefficient of different aggregated erythrocyte suspensions has been measured and correlated with the erythrocyte sedimentation rate. Finally, the size of RBC aggregates of different suspensions has been evaluated.     

Amyloid fibrils formation and amorphous aggregation in concanavalin A

We here report an experimental study on the thermal aggregation process of concanavalin A, a protein belonging to the legume lectins family. The aggregation process and the involved conformational changes of the protein molecules were followed by means of fluorescence techniques, light scattering, circular dichroism, zeta potential measurements and atomic force microscopy. Our results show that the aggregation process of concanavalin A may evolve through two distinct pathways leading, respectively, to the formation of amyloids or amorphous aggregates. The relative extent of the two pathways is determined by pH, as amyloid aggregation is favored at high pH values ( approximately 9), while the formation of amorphous aggregates is favored at low pH ( approximately 5). At difference from amorphous aggregation, the formation of amyloid fibrils requires significant conformational changes on the protein, both at secondary and tertiary structural level. To our knowledge, this is the first observation of amyloid fibrils from concanavalin A.     

Aggregation of ligand-modified liposomes by specific interactions with proteins. I: Biotinylated liposomes and avidin

The aggregation of biotin-modified phospholipid vesicles (liposomes) induced by binding the protein avidin in solution is analyzed experimentally and theoretically. Avidin has four binding sites that can recognize biotin specifically, and is able to cross-link the liposomes to form large aggregates. The aggregation kinetics were followed using quasi-elastic light scattering (QLS) to measure the mean particle size, and by measuring the solution turbidity. The rate and extent of aggregation were determined as a function of vesicle concentration, protein concentration, and the biotin density on the surface of the liposomes. A model based on Smoluchowski kinetics, fractal concepts, and Rayleigh and Mie light scattering theory was developed to analyze the experimental observations. Small aggregates (<7800 A diameter) may be treated as globular; however, the fractal nature of larger particles must be taken into account. Parameters in the model are taken from molecular simulations, or fit to the experimental observations. The aggregation kinetics are primarily determined by the biotin density on the liposome surface, the stoichiometric ratio of avidin molecules to liposomes, and the liposome concentration. Good agreement is found between the model and the experimental results. (c) 1996 John Wiley & Sons, Inc.     

Aggregation kinetics of bovine serum albumin studied by FTIR spectroscopy and light scattering

To investigate which type of structural and conformational changes is involved in the aggregation processes of bovine serum albumin (BSA), we have performed thermal aggregation kinetics in D(2)O solutions of this protein. The tertiary conformational changes are followed by Amide II band, the secondary structural changes and the formation of beta-aggregates by the Amide I' band and, finally, the hydrodynamic radius of aggregates by dynamic light scattering. The results show, as a function of pD, that: tertiary conformational changes are more rapid as pD increases; the aggregation proceeds through formation of ordered aggregates (oligomers) at pD far from the isoelectric point of the protein; disordered structures add as the pD decreases. Moreover, beta-aggregates seem to contribute only to oligomers formation, as showed by the good correlation between kinetics of scattering intensity and IR absorption intensity. These results indicate for BSA a general mechanism of aggregation composed by partial unfolding of the tertiary structure and by the decrease of alpha-helix and random coil contents in favor of beta-sheet aggregates. This mechanism strictly depends on pD and gives rise to almost two distinct types of macromolecular aggregates.     

Reconsidering the mechanism of polyglutamine peptide aggregation

There are at least nine neurodegenerative diseases associated with proteins that contain an unusually expanded polyglutamine domain, the best known of which is Huntington's disease. In all of these diseases, the mutant protein aggregates into neuronal inclusions; it is generally, although not universally, believed that protein aggregation is an underlying cause of the observed neuronal degeneration. In an effort to examine the role of polyglutamine in facilitating protein aggregation, investigators have used synthetic polyglutamine peptides as model systems. Analysis of kinetic data led to the conclusions that aggregation follows a simple nucleation-elongation mechanism characterized by a significant lag time, during which the peptide is monomeric, and that the nucleus is a monomer in a thermodynamically unfavorable conformation [Chen, S. M., et al. (2002) Proc. Natl. Acad. Sci. U.S.A. 99, 11884-11889]. We re-examined this hypothesis by measuring the aggregation kinetics of the polyglutamine peptide K2Q23K2, using sedimentation, static and dynamic light scattering, and size exclusion chromatography. Our data show that during the lag time in sedimentation kinetics, there is substantial organization of the peptide into soluble linear aggregates. These aggregates have no regular secondary structure as measured by circular dichroism but have particle dimensions and morphologies similar to those of mature insoluble aggregates. The soluble aggregates constitute approximately 30% of the total peptide mass, form rapidly, and continue to grow over a period of hours to days, eventually precipitating. Once insoluble aggregates form, loss of monomer from the solution phase continues. Our data support an assembly mechanism for polyglutamine peptide more complex than that previously proposed.     

Effect of heparin on protein aggregation: inhibition versus promotion

The effect of heparin on both native and denatured protein aggregation was investigated by turbidimetry and dynamic light scattering (DLS). Turbidimetric data show that heparin is capable of inhibiting and reversing the native aggregation of bovine serum albumin (BSA), β-lactoglobulin (BLG), and Zn-insulin at a pH near pI and at low ionic strength I; however, the results vary with regard to the range of pH, I, and protein-heparin stoichiometry required to achieve these effects. The kinetics of this process were studied to determine the mechanism by which interaction with heparin could result in inhibition or reversal of native protein aggregates. For each protein, the binding of heparin to distinctive intermediate aggregates formed at different times in the aggregation process dictates the outcome of complexation. This differential binding was explained by changes in the affinity of a given protein for heparin, partly due to the effects of protein charge anisotropy as visualized by electrostatic modeling. The heparin effect can be further extended to include inhibition of denaturing protein aggregation, as seen from the kinetics of BLG aggregation under conditions of thermally induced unfolding with and without heparin.     

Concanavalin A aggregation and toxicity on cell cultures

A number of neurodegenerative diseases are known to involve protein aggregation. Common mechanisms and structural properties of amyloids are thought to be involved in aggregation-related cytotoxicity. In this context we propose an experimental study on Concanavalin A (Con A) aggregation and use it as a model to study the relationship between cell toxicity and aggregation processes. Depending on solution conditions, Con A aggregation has been monitored by static and dynamic light scattering, Thioflavin T emission, and FTIR absorption. The morphology of different aggregate species was verified by means of Atomic Force Microscopy and Confocal Microscopy. During the aggregation pathway the native protein conformation is destabilized and as a consequence, the simultaneous occurrence of conformational changes and protein aggregation is observed in both conditions. The effects of the extracellular addition of native protein, oligomers and mature fibrils were tested on LAN5 neuroblastoma cells by MTS assay. Results showed the toxicity of the first two species while a negligible effect was detected for amyloid fibrils. Both native and oligomeric aggregates were found to be able to activate apoptosis exclusively by extrinsic pathway through caspase 8 activation. Those results suggest that cytotoxicity mechanisms arise from specific membrane interactions with reactive conformations of destabilized molecules occurring during the amyloidal aggregation pathway. Those conformations, populated when native or preformed oligomers are incubated, are unavailable to bind cell membrane proteins. This happens because they are recruited in the mature fibrillar structure which–as a consequence–turns out to be non-toxic.     

Polyglutamine repeats and β‐helix structure: Molecular dynamics study

Neurodegenerative diseases are often associated with the formation of highly insoluble aggregates. Despite the efforts devoted to the characterization of these aggregates, their structure remains elusive. Several neurodegenerative diseases are characterized by the expansion of CAG repeats, which code for Gln. Among the structural models proposed for the aggregates observed in polyQ-linked diseases, the nanotube beta-helix model proposed by Perutz and colleagues Proc Natl Acad Sci U S A 2002;99:5591-5595 has been influential. In the present study, the stability of this beta-helix model has been investigated by performing molecular dynamics simulations on polyQ fragments of different lengths. The results indicate that models shorter than two full beta-helix turns are unstable and collapse toward irregular structures. On the other hand, longer beta-helix models, containing more than 40 residues, achieve a dynamic regular structure. This finding is in line with the observed threshold of Gln repeats (approximately 40) correlated with the insurgence of the disease. Notably, the structure of the final state of the models longer than 40 residues strictly depends on their size. A compact stable ellipsoidal structure is formed by the model made of two full helical turns (41 residues), whereas water filled tubular structures emerge from simulation on longer polypeptides. These results have been interpreted taking into account the experimental data on polyQ aggregates. A structural interpretation of the literature data has been proposed by assuming that different beta-helical models are involved in the different stages of the aggregation process.     

Simulation of ultrasound backscattering by red cell aggregates: effect of shear rate and anisotropy

Tissue characterization using ultrasound (US) scattering allows extraction of relevant cellular biophysical information noninvasively. Characterization of the level of red blood cell (RBC) aggregation is one of the proposed application. In the current paper, it is hypothesized that the microstructure of the RBCs is a main determinant of the US backscattered power. A simulation model was developed to study the effect of various RBC configurations on the backscattered power. It is an iterative dynamical model that considers the effect of the adhesive and repulsive forces between RBCs, and the effect of the flow. The method is shown to be efficient to model polydispersity in size, shape, and orientation of the aggregates due to the flow, and to relate these variations to the US backscattering properties. Three levels of aggregability at shear rates varying between 0.05 and 10 s(-1) were modeled at 40% hematocrit. The simulated backscattered power increased with a decrease in the shear rate or an increase in the RBC aggregability. Angular dependence of the backscattered power was observed. It is the first attempt to model the US power backscattered by RBC aggregates polydisperse in size and shape due to the shearing of the flow.     

Experimental study on aggregation of model dipeptide molecules. V. Stereoselective association of leucine dipeptides

Infrared spectroscopy and ¹H nmr have been used to elucidate the association modes of leucine dipeptides in carbon tetrachloride solution. Two stereoselective types of aggregates have been evidenced. Homochiral molecules are associated in oligomeric aggregates and accommodate a β-parallel-like structure which was characterized by x-ray diffraction. Heterochiral molecules are paired in centrosymmetrical dimers; the latter aggregation mode restricted to the dimer stage predominates in racemic solutions. A theoretical model proposed to account for this aggregation process is consistent with the experimental nmr data. Both homo- and heterochiral association constants are estimated from vapor pressure and nmr experiments.     

Effect of α-crystallin on thermal aggregation of glycogen phosphorylase <Emphasis Type="Italic">b</Emphasis> from rabbit skeletal muscle

Thermal aggregation of rabbit skeletal muscle glycogen phosphorylase b (Phb) has been investigated using dynamic light scattering under conditions of a constant rate of temperature increase (1 K/min). The linear behavior of the dependence of the hydrodynamic radius on temperature for Phb aggregation is consistent with the idea that thermal aggregation of proteins proceeds in the kinetic regime wherein the rate of aggregation is limited by diffusion of the interacting particles (the regime of "diffusion-limited cluster-cluster aggregation"). In the presence of alpha-crystallin, a protein exhibiting chaperone-like activity, the dependence of the hydrodynamic radius on temperature follows the exponential law; this suggests that the aggregation process proceeds in the kinetic regime where the sticking probability for colliding particles becomes lower than unity (the regime of "reaction-limited cluster-cluster aggregation"). Based on analysis of the ratio between the light scattering intensity and the hydrodynamic radius of Phb aggregates, it has been concluded that the addition of alpha-crystallin results in formation of smaller size starting aggregates. The data on differential scanning calorimetry indicate that alpha-crystallin interacts with the intermediates of the unfolding process of the Phb molecule. The proposed scheme of thermal denaturation and aggregation of Phb includes the stage of reversible dissociation of dimers of Phb into monomers, the stage of the formation of the starting aggregates from the denatured monomers of Phb, and the stage of the sticking of the starting aggregates and higher order aggregates. Dissociation of Phb dimer into monomers at elevated temperatures has been confirmed by analytical ultracentrifugation.     

Solution structure of copper ion-induced molecular aggregates of tyrosine melanin.

Melanin, the ubiquitous biological pigment, provides photoprotection by efficient filtration of light and also by its antioxidant behavior. In solutions of synthetic melanin, both optical and antioxidant behavior are affected by the aggregation states of melanin. We have utilized small-angle x-ray and neutron scattering to determine the molecular dimensions of synthetic tyrosine melanin in its unaggregated state in D(2)O and H(2)O to study the structure of melanin aggregates formed in the presence of copper ions at various copper-to-melanin molar ratios. In the absence of copper ions, or at low copper ion concentrations, tyrosine melanin is present in solution as a sheet-like particle with a mean thickness of 12.5 A and a lateral extent of approximately 54 A. At a copper-to-melanin molar ratio of 0.6, melanin aggregates to form long, rod-like structures with a radius of 32 A. At a higher copper ion concentration, with a copper-to-melanin ratio of 1.0, these rod-like structures further aggregate, forming sheet-like structures with a mean thickness of 51 A. A change in the charge of the ionizable groups induced by the addition of copper ions is proposed to account for part of the aggregation. The data also support a model for the copper-induced aggregation of melanin driven by pi stacking assisted by peripheral Cu(2+) complexation. The relationship between our results and a previous hypothesis for reduced cellular damage from bound-to-melanin redox metal ions is also discussed.     

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.     

Differential scattering of circularly polarized light as a unique probe of polynucleosome superstructures

A theoretical approach to modeling Circular Intensity Differential Scattering (CIDS) of native chromatin as multiple scattering of dipoles is discussed without the Born approximation. The model can explain the experimental data in the literature. It is shown that CIDS contains more structural information than does total light scattering and to a good approximation is independent of the length of the scattering molecules. Finally, CIDS in conjunction with traditional light scattering measurements should aid in discriminating between various alternative models of higher order chromatin structure now being proposed. Generalization of this theoretical study to other complex biomolecular structures, is also briefly discussed.     

Thermo- and photoinduced aggregation of alpha-crystallin

Some properties of bovine alpha-crystallin, in particular its thermo- and photoaggregation, were studied by fluorescent spectroscopy of tryptophan residues and the probe 8-anilino-1-naphthalenesulfonate and light scattering. The effective diameter of a globule of native alpha-crystallin was 90 A, as estimated from the data on the polarization and lifetime of 8-anilino-1-naphthalenesulfonate using the Levshin-Perren equation, and increases at an aggregation of no less than 140 A. The increase in the intensity of tryptophan fluorescence of alpha-crystallin during its thermo- and photodenaturation with the formation of aggregates is due to local conformational changes in the surroundings of tryptophan residues and light scattering. Tryptophan residues are buried in the interior of the aggregates. The thermoaggregation of the protein occurs not only at high temperatures. By approximating the experimental time dependence of slow spontaneous aggregation to the range of large times, the time of denaturation aggregation t(e) was found. For alpha-crystallin (at a concentration of 0.8 mg/ml in phosphate buffer at pH 8.4), t(e) at 70 degrees C is 100 h. This approach can be used in finding t(e) for any protein during its thermal treatment or long-term storage.     

Differential scattering of circularly polarized light as a unique probe of polynucleosome superstructures. A simulation by multiple scattering of dipoles

A theoretical approach to modeling Circular Intensity Differential Scattering (CIDS) of native chromatin as multiple scattering of dipoles is discussed without the Born approximation. The model can explain the experimental data in the literature. It is shown that CIDS contains more structural information than does total light scattering and to a good approximation is independent of the length of the scattering molecules. Finally, CIDS in conjunction with traditional light scattering measurements should aid in discriminating between various alternative models of higher order chromatin structure now being proposed. Generalization of this theoretical study to other complex biomolecular structures, is also briefly discussed.     

Colloidal properties of human transferrin receptor in detergent free solution

The colloidal properties of transferrin receptor, isolated from human placenta, in detergent free solution has been investigated by light scattering techniques and analytical ultracentrifugation. In detergent free solution at 293.2 K, hTfR forms stable aggregates with an apparent hydrodynamic radius of 17 nm. The molecular mass was determined by ultracentrifugation to lie between (1722+/-87) kDa (sedimentation equilibrium) and (1675+/-46) kDa (sedimentation velocity). This implies that the aggregates are build up from nine hTfR dimers. Based on model calculations, which are in good agreement with the experimental data, we propose a torus-like structure for the aggregates. Upon pH shift from pH 7.5 to 5.0 or removal of the N-linked carbohydrate chains, formation of larger aggregates is induced. These aggregates can be described in terms of porous fractal structures. We propose a simple model, which accounts for that behaviour assuming that the aggregation is mainly due to the reduction of negative surface charge.     

The role of the immunoglobin G "hinge" region in heat aggregation and activation of complex-formation

A high degree of correlation between the capability of subclasses of human immunoglobulins G to form aggregates due to thermal treatment, and their complement-binding activity was established. On the basis of the experimental data obtained by the methods of light scattering, circular dichroism, microcalorimetry, it was supposed that "hinge" region of immunoglobulins G participates in the initial stage of thermal aggregation and in the activation of the process of complement binding.     

Examining Polyglutamine Peptide Length: A Connection between Collapsed Conformations and Increased Aggregation

Abnormally expanded polyglutamine domains in proteins are associated with several neurodegenerative diseases, of which the best known is Huntington's. Expansion of the polyglutamine domain facilitates aggregation of the affected protein, and several studies directly link aggregation to neurotoxicity. The age of onset of disease is inversely correlated with the length of the polyglutamine domain; this correlation motivates an examination of the role of the length of the domain on aggregation. In this investigation, peptides containing 8 to 24 glutamines were synthesized, and their conformational and aggregation properties were examined. All peptides lacked secondary structure. Fluorescence resonance energy transfer studies revealed that the peptides became increasingly collapsed as the number of glutamine residues increased. The effective persistence length was estimated to decrease from ∼ 11 to ∼ 7 Å as the number of glutamines increased from 8 to 24. A comparison of our data with theoretical results suggests that phosphate-buffered saline is a good solvent for Q8 and Q12, a theta solvent for Q16, and a poor solvent for Q20 and Q24. By dynamic light scattering, we observed that Q16, Q20, and Q24, but not Q8 or Q12, immediately formed soluble aggregates upon dilution into phosphate-buffered saline at 37 °C. Thus, Q16 stands at the transition point between good and poor solvent and between stable and aggregation-prone peptide. Examination of aggregates by transmission electron microscopy, along with kinetic assays for sedimentation, provided evidence indicating that soluble aggregates mature into sedimentable aggregates. Together, the data support a mechanism of aggregation in which monomer collapse is accompanied by formation of soluble oligomers; these soluble species lack regular secondary structure but appear morphologically similar to the sedimentable aggregates into which they eventually mature.