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.     

Swelling and dissolution of beta-lactoglobulin gels in alkali

It is well documented in the literature that during the dissolution of whey protein gels in alkali, the gels swell to a great extent. However, the relevance of the swelling step in the dissolution process of the protein gel remains unknown. In the present article we present a systematic study on the swelling of beta-lactoglobulin gels at different alkaline pH and ionic strengths. The equilibrium swelling degree at different conditions has been modeled using a simple model developed for polyelectrolyte gels, modified to take into account the ionization of the residues in a protein. The model can describe the swelling behavior of the gels over a wide range of conditions, but it underpredicts the equilibrium swelling under conditions close to those when dissolution is observed. Dissolution is only noticeable above pH 11.5-12 and only for those gels that are swollen over a minimum degree, suggesting the existence of a dissolution threshold.     

Effects of amylopectin structure and molecular weight on microstructural and rheological properties of mixed beta-lactoglobulin gels

Nongelling amylopectin fractions from potato and barley have been used to form mixed beta-lactoglobulin gels. The amylopectin fractions were produced by varying the time of alpha-amylase hydrolysis followed by sequential ethanol precipitation. The molecular weights, radius of gyration, chain length distribution, and viscosity of the fractions were established. The mixed gels were analyzed rheologically with dynamic mechanical analysis in shear and microstructurally with light microscopy, transmission electron microscopy, and nuclear magnetic resonance spectroscopy. The result of the gel studies clearly showed that small differences in the molecular weight of amylopectins have a significant influence on the kinetics of protein aggregation and thereby on the gel microstructure and the rheological behavior of the gel. Both an increase in the molecular weight and a higher concentration of amylopectins resulted in a more open protein network structure, with thicker strands of larger and more close-packed beta-lactoglobulin clusters, which showed a larger storage modulus. The transmission electron micrographs revealed that degraded amylopectins were enclosed inside the protein clusters in the mixed gels, whereas nondegraded amylopectin was only found outside the protein clusters. The volume-weighted mean value of the molecular weight of the amylopectins was found to vary between 3.2 x 10(4) and 5.0 x 10(7) Da and the ratio of gyration between 14 and 61 nm. The maximum in chain length distribution was generally somewhat distributed toward longer chain lengths for potato compared to barley, but the differences in chain length distribution were minor compared to those seen in the molecular weight and ratio of gyration between the fractions.     

The pH threshold in the dissolution of beta-lactoglobulin gels and aggregates in alkali

The existence of a practical minimum pH for the dissolution of heat-induced whey gels in alkaline solutions has been studied using beta-lactoglobulin (betaLg) as a model protein. A sharp transition in solubility was observed between pH 11 and 12; this transition shifts to higher pHs for gels formed at higher temperatures and for longer gelling times. The breakdown reactions of heat-induced aggregates in alkali were monitored with size exclusion chromatography. The destruction of large aggregates was faster at higher pH and also showed a transition between pH 11 and 12. Using tryptophan fluorescence and near- and far-UV circular dichroism, this transition was assigned to the base-induced denaturation observed in solutions of aggregates (pK 11.53). It is suggested that the high protein repulsion caused by the large number of charges at pH > 11.5 drives the unfolding of the protein and the disruption of the intermolecular noncovalent bonds. Concentrated urea and GuHCl were found to be less effective than a pH 12 solution in destroying large aggregates. Aggregates formed for a long time (80 degrees C for 24 h) contained a larger number of intermolecular disulfide bonds that hinder the dissolution process. Gels formed at low temperatures (65 degrees C for 60 min), with fewer intermolecular noncovalent bonds, showed a similar solubility-pH profile to that observed for the base-induced denaturation of unheated beta-lactoglobulin (betaLg) (pK 10.63).     

Heat-induced gelation of globular proteins: part 3. Molecular studies on low pH beta-lactoglobulin gels

Heat-set gels and aggregates from beta-lactoglobulin (beta-Lg), one of the major globular proteins from milk, have been studied on a molecular distance scale using negative-staining transmission electron microscopy (TEM), wide-angle X-ray diffraction (WAXD), and Fourier transform infrared spectroscopy (FTIR). The microscopy showed long linear aggregates forming in solutions at pH 2 (and sometimes 2.5) after prolonged heating. While there appeared to be no differences in aggregates formed under these conditions in H(2)O as compared with D(2)O, at all other pH and pD values, and in the presence of added salt, much shorter linear aggregates were formed. These became slightly more extended the further the pH was removed from pI. Wide-angle X-ray diffraction (WAXD) showed a diffuse beta-sheet halo at 2θ=19 degrees in patterns for both dried native and aggregated protein (irrespective of pH) with only a small change (sharpening) of this feature on heat treatment. Solution FTIR spectra, measured at pD=2, 2.5, 3, and 7, during heating, indicated shoulder development at 1612 cm(-1) in the carbonyl-stretching Amide I region diagnostic of a modest increase in intermolecular beta-sheet. In terms of the shoulder size, no distinctions could be made between acid and neutral aggregate structures. At all pHs, beta-lactoglobulin showed only limited secondary and tertiary structural changes in aggregation, in contrast to previous studies of insulin aggregation, where highly ordered crystalline fibrils were indicated. The current work has implications both in structural studies of food biopolymers and in ongoing studies of pathological protein self-assembly in disease states, such as spongiform encephalopathies.     

Interactions responsible for secondary structure formation during folding of equine beta-lactoglobulin

Equine beta-lactoglobulin forms a compact intermediate at an acidic pH (A state). It also forms an expanded and helical conformation at low temperatures (C state). The structure of a single disulfide mutant C66A/C160A is similar to the A state in the presence of salts, while it is similar to the C state at low anion concentrations. We have investigated the temperature-dependent change in the secondary structure using circular dichroism and proline scanning mutagenesis. At low anion concentrations, the helical content increased linearly as temperature decreased. In the presence of salts, the A state was cooperatively transformed into the C state at low temperatures. This suggests the importance of hydrophobic interactions for stabilizing the A state. Peptides encompassing native-like and non-native alpha-helices were synthesized to investigate the interactions responsible for helix formation in the A and C states. These did not form stable helices, indicating that not only the helices in the A state but also the helices in the C state are stabilized by long-range interactions. A longer fragment, CHIBL, which encompasses the structured region in the A and C states, showed a helical structure. Proline-substituted mutants of CHIBL showed CD spectral changes similar to the corresponding mutants of the full-length protein in the C state. Therefore, CHIBL has a structure similar to the corresponding region of the full-length protein in the C state. This result indicates that interactions responsible for helix formation in the C state reside in the sequence of CHIBL, and that the sequences outside CHIBL are essential for secondary structure formation in the A state.     

Effect of electrostatic interactions on the percolation concentration of fibrillar beta-lactoglobulin gels

The effect of electrostatic interactions on the critical percolation concentration (c(p)) of fibrillar beta-lactoglobulin gels at pH 2 was investigated using rheological measurements, transmission electron microscopy (TEM), and performing conversion experiments. A decreasing c(p) with increasing ionic strength was found. The fraction of nonaggregated beta-lactoglobulin was independent of ionic strength in the regime of 0.01-0.08 M. TEM experiments showed long fibrils (2-7 microm) for ionic strengths between 0.01 and 0.08 M. Since both the conversion of monomers and the contour length of the fibrils were independent of ionic strength (0.01-0.08M), the linear increase of c(p) with the Debye length can be attributed purely to an increase of electrostatic repulsion between the fibrils. This increase is explained in terms of an adjusted random contact model which takes into account the charge and semiflexibility of the fibrils.     

Molecular cloning of bovine beta-lactoglobulin cDNA

A cDNA library from bovine mammary gland mRNA was constructed in pBR322 and screened by hybrid-selected translation and immunoscreening. Several beta-lactoglobulin clones were identified and sequenced. All clones contained cDNA fragments corresponding to the 3' region of beta-lactoglobulin mRNA. The 3' non-translated region of beta-lactoglobulin mRNA consists of 187 nucleotides; the polyadenylation signal AATAAA occurs 17 nucleotides before the poly(A) tail. The amino-acid sequence predicted from the 3' coding region corresponds completely to the previously determined amino-acid sequence of beta-lactoglobulin.     

Multiple steps during the formation of beta-lactoglobulin fibrils

In this study, the heat induced fibrilar aggregation of the whey protein beta-lactoglobulin is investigated at low pH and at low ionic strength. Under these circumstances, tapping mode atomic force microscopy results indicate that the fibrils formed have a periodic structure with a period of about 25 nm and a thickness of one or two protein monomers. Fibril formation is followed in situ using light scattering and proton NMR techniques. The dynamic light scattering results show that the fibrils that form after short heating periods (up to a few hours) disintegrate upon slow cooling, whereas fibrils that form during long heating periods do not disintegrate upon subsequent slow cooling. The NMR results show that even after prolonged heating an appreciable fraction of the protein molecules is incorporated into fibrils only when the beta-lactoglobulin concentration is above approximately 2.5 wt %. The data imply multiple steps during the heat induced formation of beta-lactoglobulin fibrils at low pH and at low ionic strength: (partly) denatured protein monomers are either incorporated into fibrils or form instead a low molecular weight complex that is incapable of forming fibrils. Fibril formation itself also involves (at least) two steps: the reversible formation of linear aggregates, followed by a slow process of "consolidation" after which the fibrils no longer disintegrate upon slow cooling.     

Molecular dynamics simulations of the whey protein beta-lactoglobulin.

Molecular dynamics simulations have been used to model the motions and conformational behavior of the whey protein bovine beta-lactoglobulin. Simulations were performed for the protein by itself and complexed to a single retinol ligand located in a putative interior binding pocket. In the absence of the retinol ligand, the backbone loops around the opening of this interior pocket shifted inward to partially close off this cavity, similar to the shifts observed in previously reported molecular dynamics simulations of the uncomplexed form of the homologous retinol binding protein. The protein complexed with retinol does not exhibit the same conformational shifts. Conformational changes of this type could serve as a recognition signal allowing in vivo discrimination between the free and retinol complexed forms of the beta-lactoglobulin molecule. The unusual bending of the single alpha-helix observed in the simulations of retinol binding protein were not observed in the present calculations.     

Secondary structure of bovine beta-lactoglobulin B

Secondary-structure-prediction algorithms have been used to find the segments of beta-lactoglobulin sequence most likely to fit the circular dichroism assignment of 15% alpha-helix, 50% beta-sheet, and 15-20% reverse turn. A number of segments may have an alpha-helical conformation but the most prominent region of alpha-helix is from residue 129 to 143. A further probable alpha-helix segment is residues 65-76. The number of residues predicted to occur in segments of beta-sheet structure is less than expected. However, the most likely segments are for residues 1-6, 11-16, 39-45, 80-85, 92-96, 101-107, 117-123, and 145-151. Predicted reverse-turn tetrapeptides are residues 7-10, 49-52, 61-64, 88-91, and 112-115. These predicted secondary structures are consistent with the low-resolution structure of the molecule determined by X-ray diffraction studies.     

Circular dichroism study on the early folding events of beta-lactoglobulin entrapped in wet silica gels

beta-Lactoglobulin is a predominantly beta-sheet protein that folds by forming excess alpha-helices within milliseconds. In this study, the refolding of beta-lactoglobulin was dramatically decelerated by entrapping in wet nanoporous silica gel matrices, and monitored on a time scale of minutes or hours by far-UV circular dichroism spectroscopy. Analysis of kinetics and transient spectra allowed to define the sequence of folding events that consist of alpha-helical formation, beta-sheet core formation, and alpha-to-beta transition. The results suggest that the initially formed alpha-helices, presumably including the native alpha-helix, help to guide the formation of the adjacent beta-sheet core.     

Changes in structure and in interactions of heat-treated bovine beta-lactoglobulin

Heat stress on structure and ligand binding of beta-LG has been studied by fluorescence, circular dichroism and gel electrophoresis at pH 6.5. Native PAGE gel electrophoresis shows that denaturation of beta-LG is reversible up to 75 degrees C then it becomes irreversible due to aggregation of beta-LG. Formation of aggregated beta-LG is completed at 95 degrees C. Circular dichroism results indicate that formation of aggregated beta-LG is accompanied by the scrambling of disulfide bonds (creation of new intramolecular and intermolecular disulfide bridges and rearrangement of old intramolecular disulfide bridges). Addition of ethanolic retinol causes a change in polarity of the solution and favors transformation of the beta<-->alpha structure. In the presence of retinol, the alpha-helix content of the secondary structure of heat-treated beta-LG is increased and the major portion of its secondary structure is helical. Fluorescence results show that heat-treated beta-LG at 95 degrees C can still bind retinol. The refolding of the tertiary structure of beta-LG heat-denatured at 95 degrees C may recreate a retinol binding site. Surprisingly, the affinity of the new site for retinol is higher than that of native beta-LG; however, the apparent molar ratio is lower than one. The binding properties of beta-LG for terpenoids have been measured after its heat treatment at 20, 75 and 95 degrees C. The intensity of tryptophan emission at 330 nm was changed only in the case of the interaction with beta-ionone. Other ligands probably cannot bind to beta-LG or they bind in a binding site far from the tryptophan residues, hence not affecting its fluorescence.     

Solution structure and dynamics of bovine beta-lactoglobulin A

Using heteronuclear NMR spectroscopy, we studied the solution structure and dynamics of bovine beta-lactoglobulin A at pH 2.0 and 45 degrees C, where the protein exists as a monomeric native state. The monomeric NMR structure, comprising an eight-stranded continuous antiparallel beta-barrel and one major alpha-helix, is similar to the X-ray dimeric structure obtained at pH 6.2, including betaI-strand that forms the dimer interface and loop EF that serves as a lid of the interior hydrophobic hole. [1H]-15N NOE revealed that betaF, betaG, and betaH strands buried under the major alpha-helix are rigid on a pico- to nanosecond time scale and also emphasized rapid fluctuations of loops and the N- and C-terminal regions.     

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.     

Molecular interactions between a recombinant IgE antibody and the beta-lactoglobulin allergen

Allergies are caused by the immune reaction to commonly harmless proteins, allergens. This reaction is typified by immunoglobulin E (IgE) antibodies. We report the crystal structure of an IgE Fab fragment in complex with beta-lactoglobulin (BLG), one of the major allergens of bovine milk. The solved structure shows how two IgE/Fab molecules bind the dimeric BLG. The epitope of BLG consists of six different short fragments of the polypeptide chain, which are located especially in the beta strands, covering a flat area on the allergen surface. All six CDR (complementary-determining region) loops of the IgE Fab participate in the binding of BLG. The light chain CDR loops are responsible for the binding of the flat beta sheet region of BLG. The IgE epitope is different from common IgG epitopes that are normally located in the exposed loop regions of antigens and observed also in the two recently determined allergen-IgG complexes.     

Molecular description of the formation and structure of plasticized globular protein films

To optimize the properties of plasticized globular proteins films, a clear comprehension of the structure and molecular events occurring during film formation is required. In this work, the structural organization of beta-lactoglobulin (beta-lg) films plasticized with diethyelene glycol are investigated for the first time during the entire film formation process by attenuated total reflectance and transmission infrared spectroscopy. The films are made by a common two-step procedure consisting of a first heat treatment (80 degrees C/30 min) followed by the casting of the film-forming solution for dehydration. Heating at 80 degrees C leads to the self-aggregation of the proteins with a conversion of regular secondary structures into antiparallel beta-sheets. The kinetics of the conformational conversion shows that approximately 10% of the amino acids are involved in beta-sheets after the first step. Dehydration induces a further aggregation, with approximately 46% of the amino acids involved in beta-sheets in the final film. Water evaporation results in the association of the aggregates formed during the heating step. The presence of the plasticizer during water removal is essential as it allows specific conformational rearrangements into extended beta-sheets and ordering of the polypeptide chains. This work underlines that the assembly of building blocks is common in beta-lg networks and it emphasizes the widespread occurrence of beta-structures in synthetic and natural protein networks.