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.     

Similar toxicity of the oligomeric molten globule state and the prefibrillar oligomers

We report that a mutant of human stefin B is in a molten globule conformation. It has all the spectroscopic characteristics for such a state. We also demonstrate that the molten globule is oligomeric, eluting on SEC within a similar MW range than the higher order oligomers of the wild type protein, which is confirmed by DLS and AFM. Both, the higher oligomers and the molten globule state bind ANS, implying a high degree of hydrophobic patches exposure and partial opening of the structure. Finally, we demonstrate that the oligomeric molten globule is as toxic as the prefibrillar aggregates obtained at acid pH or the higher order oligomers prepared at neutral pH.     

Factors determining pressure perturbation calorimetry measurements: evidence for the formation of metastable states at lipid phase transitions

The factors that influence the application of pressure perturbation calorimetry in studying the volume change of the phase transition of lipids are discussed. These factors include a correction for the temperature-shift induced by perturbation, the kinetic irreversibility of the phase transition and the magnitude of the pressure perturbation. We take into account the fact that the dependence of the phase transition temperature on pressure will affect the temperature-shift induced by pressure. As a result, there is a discrepancy between the compression part of the cycle and the expansion. In addition, sequential cycles lead to a gradual loss in magnitude of the heat effect upon pressure perturbation. We suggest that these phenomena can be explained by the formation of a metastable glass-like state that converts to a stable phase at temperatures removed from the region of the phase transition.     

Evidence for stepwise formation of amyloid fibrils by the mouse prion protein

The full-length mouse prion protein, moPrP, is shown to form worm-like amyloid fibrils at pH 2 in the presence of 0.15 M NaCl, in a slow process that is accelerated at higher temperatures. Upon reduction in pH to 2, native moPrP transforms into a mixture of soluble β-rich oligomers and α-rich monomers, which exist in a slow, concentration-dependent equilibrium with each other. It is shown that only the β-rich oligomers and not the α-rich monomers, can form worm-like amyloid fibrils. The mechanism of formation of the worm-like amyloid fibrils from the β-rich oligomers has been studied with four different physical probes over a range of temperatures and over a range of protein concentrations. The observed rate of fibrillation is the same, whether measured by changes in ellipticity at 216 nm, in thioflavin fluorescence upon binding, or in the mean hydrodynamic radius. The observed rate is significantly slower when monitored by total scattering intensity, suggesting that lateral association of the worm-like fibrils occurs after they form. The activation energy for worm-like fibril formation was determined to be 129 kJ/mol. The observed rate of fibrillation increases with an increase in protein concentration, but saturates at protein concentrations above 50 μM. The dependence of the observed rate of fibrillation on protein concentration suggests that aggregate growth is rate-limiting at low protein concentration and that conformational change, which is independent of protein concentration, becomes rate-limiting at higher protein concentrations. Hence, fibril formation by moPrP occurs in at least two separate steps. Longer but fewer worm-like fibrils are seen to form at low protein concentration, and shorter but more worm-like fibrils are seen to form at higher protein concentrations. This observation suggests that the β-rich oligomers grow progressively in size to form critical higher order-oligomers from which the worm-like amyloid fibrils then form.     

Conformational Conversion May Precede or Follow Aggregate Elongation on Alternative Pathways of Amyloid Protofibril Formation

A major goal in the study of protein aggregation is to understand how the conformational heterogeneity characteristic of the process leads to structurally distinct amyloid fibrils. The small protein barstar is known to form amyloid protofibrils in multiple steps at low pH: a small oligomer, the A-form, first transforms into a larger spherical higher oligomeric intermediate (HOI), which then self-associates to form the elongated protofibril. To determine how the conformational conversion reaction during aggregation is coupled to the process of protofibril formation, cysteine-scanning mutagenesis was first used to identify specific residue positions in the protein sequence, which are important in defining the nature of the aggregation process. Two classes of mutant proteins, which are distinguished by their kinetics of aggregation at high protein concentration, have been identified: Class I mutant proteins undergo conformational conversion, as measured by an increase in thioflavin T binding ability and an increase in circular dichroism at 216 nm, significantly faster than Class II mutant proteins. At low protein concentration, the rates of conformational conversion are, however, identical for both classes of mutant proteins. At high protein concentration, the two classes of mutant proteins can be further distinguished on the basis of their rates of protofibril growth, as determined from dynamic light-scattering measurements. For Class I mutant proteins, protofibril elongation occurs at the same, or slightly faster, rate than conformational conversion. For Class II mutant proteins, protofibril elongation is significantly slower than conformational conversion. Dynamic light scattering measurements and atomic force microscopy imaging indicate that for the Class I mutant proteins, conformational conversion occurs concurrently with the self-association of prefibrillar HOIs into protofibrils. On the other hand, for the Class II mutant proteins, the prefibrillar HOI first undergoes conformational conversion, and the conformationally converted HOIs then self-associate to form protofibrils. The two classes of mutant proteins appear, therefore, to use structurally distinct pathways to form amyloid protofibrils. On one pathway, conformational conversion occurs along with, or after, elongation of the oligomers; on the other pathway, conformational conversion precedes elongation of the oligomers. Single mutations in the protein can cause aggregation to switch from one pathway to the other. Importantly, the protofibrils formed by the two classes of mutant proteins have significantly different diameters and different internal structures.     

Periodically arranged interactions within the myosin filament backbone revealed by mechanical unzipping

Numerous types of biological motion are driven by myosin thick filaments. Although the exact structure of the filament backbone is not known, it has long been hypothesized that periodically arranged charged regions along the myosin tail are the main contributors to filament stability. Here we provide a direct experimental test of this model by mechanically pulling apart synthetic myosin thick filaments. We find that unzipping is accompanied by broad force peaks periodically spaced at 4-, 14- and 43-nm intervals. This spacing correlates with the repeat distance of highly charged regions along the myosin tail. Lowering ionic strength does not change force-peak periodicity but increases the forces necessary for unzipping. The force peaks are partially reversible, indicating that the interactions are rapidly re-established upon mechanical relaxation. Thus, the zipping together of myosin tails via consecutive formation of periodically spaced bonds may be the underlying mechanism of spontaneous thick filament formation.     

The two-fold aspect of the interplay of amyloidogenic proteins with lipid membranes

Investigating the pathways leading to the formation of amyloid protein aggregates and the mechanism of their cytotoxicity is fundamental for a deeper understanding of a broad range of human diseases. Increasing evidence indicates that early aggregates are responsible for the cytotoxic effects. This paper addresses the catalytic role of lipid surfaces in promoting aggregation of amyloid proteins and the permeability changes that these aggregates induce on lipid membranes. Effects of amyloid aggregates on model systems such as monolayers, vesicles, liposomes and supported lipid bilayers are reviewed. In particular, the relevance of atomic force microscopy in detecting both kinetics of amyloid formation and amyloid-membrane interactions is emphasized.     

Negatively charged phospholipid membranes induce amyloid formation of medin via an alpha-helical intermediate

Medin, a recently discovered 5.5 kDa peptide, is associated with amyloid deposits in the medial layer of human arteries and the prevalence is nearly 100% within individuals above 50 years. Presently, not much is known about its biochemical and biophysical properties or its pathway from soluble peptide to insoluble amyloid. Here we have characterized the behavior of medin in the presence of lipid membranes, using circular dichroism, isothermal titration calorimetry, differential scanning calorimetry, size exclusion chromatography, and atomic force microscopy (AFM). Medin was shown to exist as a monomer in solution with a predominantly random-coil structure. It binds lipid vesicles that have either a neutral or a negative surface potential. Upon association to membranes containing acidic lipids, it undergoes an electrostatically driven conformational change towards a mainly α-helical state. Prolonged incubation converts medin from an α-helical structure into an amyloid β-sheet fibrillar state as confirmed by AFM. Based on these findings, we propose a mechanism of medin-amyloid formation where medin electrostatically associates in its monomeric form to biological interfaces displaying a negative potential. This process both increases the local peptide concentration and induces an aggregation-prone α-helical fold.     

Folding and assembly of proteorhodopsin

Proteorhodopsins (PRs), the recently discovered light-driven proton pumps, play a major role in supplying energy for microbial organisms of oceans. In contrast to PR, rhodopsins found in Archaea and Eukarya are structurally well characterized. Using single-molecule microscopy and spectroscopy, we observed the oligomeric assembly of native PR molecules and detected their folding in the membrane. PR showed unfolding patterns identical with those of bacteriorhodopsin and halorhodopsin, indicating that PR folds similarly to archaeal rhodopsins. Surprisingly, PR predominantly assembles into hexameric oligomers, with a smaller fraction assembling into pentamers. Within these oligomers, PR arranged into radial assemblies. We suggest that this structural assembly of PR may have functional implications.     

A comparative study of the effect of cholesterol on bicelle model membranes using X-band and Q-band EPR spectroscopy

X-band and Q-band electron paramagnetic resonance (EPR) spectroscopic techniques were used to investigate the structure and dynamics of cholesterol containing phospholipid bicelles based upon molecular order parameters (S_mol), orientational dependent hyperfine splittings and line shape analysis of the corresponding EPR spectra. The nitroxide spin-label 3-β-doxyl-5-α-cholestane (cholestane) was incorporated into DMPC/DHPC bicelles to report the alignment of bicelles in the static magnetic field. The influence of cholesterol on aligned phospholipid bicelles in terms of ordering, the ease of alignment, phase transition temperature have been studied comparatively at X-band and Q-band. At a magnetic field of 1.25 T (Q-band), bicelles with 20 mol% cholesterol aligned at a much lower temperature (313 K), when compared to 318 K at a 0.35 T field strength for X-band, showed better hyperfine splitting values (18.29 G at X-band vs. 18.55 G at Q-band for perpendicular alignment and 8.25 G at X-band vs. 7.83 G at Q-band for the parallel alignment at 318 K) and have greater molecular order parameters (0.76 at X-band vs. 0.86 at Q-band at 318 K). Increasing cholesterol content increased the bicelle ordering, the bicelle-alignment temperature and the gel to liquid crystalline phase transition temperature. We observed that Q-band is more effective than X-band for studying aligned bicelles, because it yielded a higher ordered bicelle system for EPR spectroscopic studies.     

Improved model systems for bacterial membranes from differing species: The importance of varying composition in PE/PG/cardiolipin ternary mixtures

Abstract

Steady-state fluorescence anisotropy and dynamic light scattering (DLS) were used to determine the thermotropic properties of lipid systems that act as models for bacterial membranes of Yersinia kristensenii and Proteus mirabilis. Lipid proportions of PE:PG:CL of 0.60:0.20:0.20 and 0.80:0.15:0.05, were used in order to mimic these two membranes respectively. We observed that the introduction of cardiolipin (CL) as a third lipid component of any PE:PG mixture, changes the system's properties considerably. The results obtained by these two techniques show that the main transition temperatures obtained are undoubtedly CL-dependent. Additionally AFM experiments were performed and these results show that even at small concentration CL produces important changes not only in the membrane thermotropic properties, but also in the bilayer structure. In summary, we were able to compare how low and high CL concentration affect bacterial membrane model system properties which can provide a further explanation for the different antibiotic susceptibilities reported for Y. kristensenii and P. mirabilis.     

Loading a ring: structure of the Bacillus subtilis DnaB protein, a co-loader of the replicative helicase

Loading of the ring-shaped replicative helicase is a critical step in the initiation of DNA replication. Bacillus subtilis has adopted a two-protein strategy to load its hexameric replicative helicase: DnaB and DnaI interact with the helicase and mediate its delivery onto DNA. We present here the 3D electron microscopy structure of the DnaB protein, along with a detailed analysis of both its oligomeric state and its domain organization. DnaB is organized as an asymmetric tetramer that is comprised of two stacked components, one arranged as a closed collar and the other as an open sigma shape. Intriguingly, the 3D map of DnaB exhibits an overall architecture similar to the structure of the Escherichia coli gamma-complex, the loader of the ring-shaped processivity factor. We propose a model whereby each DnaB monomer participates in both stacked components of the tetramer and displays a different overall shape. This asymmetric quaternary organization could be a general feature of ring loaders.     

Probing Interactions within the synaptic DNA-SfiI complex by AFM force spectroscopy

SfiI belongs to a family of restriction enzymes that function as tetramers, binding two recognition regions for the DNA cleavage reaction. The SfiI protein is an attractive and convenient model for studying synaptic complexes between DNA and proteins capable of site-specific binding. The enzymatic action of SfiI has been very well characterized. However, the properties of the complex before the cleavage reaction are not clear. We used single-molecule force spectroscopy to analyze the strength of interactions within the SfiI-DNA complex. In these experiments, the stability of the synaptic complex formed by the enzyme and two DNA duplexes was probed in a series of approach-retraction cycles. In order to do this, one duplex was tethered to the surface and the other was tethered to the probe. The complex was formed by the protein present in the solution. An alternative setup, in which the protein was anchored to the surface, allowed us to probe the stability of the complex formed with only one duplex in the approach-retraction experiments, with the duplex immobilized at the probe tip. Both types of complexes are characterized by similar rupture forces. The stability of the complex was determined by measuring the dependence of rupture forces on force loading rates (dynamic force spectroscopy) and the results suggest that the dissociation reaction of the SfiI-DNA complex has a single energy barrier along the dissociation path. Dynamic force spectroscopy was instrumental in revealing the role of the 5 bp spacer region within the palindromic recognition site on DNA-SfiI in the stability of the complex. The data show that, although the change of non-specific sequence does not alter the position of the activation barrier, it changes values of the off rates significantly.     

Sphingomyelinase generation of ceramide promotes clustering of nanoscale domains in supported bilayer membranes

The effects of ceramide incorporation in supported bilayers prepared from ternary lipid mixtures which have small nanoscale domains have been examined using atomic force and fluorescence microscopy. Both direct ceramide incorporation in vesicles used to prepare the supported bilayers and enzymatic hydrolysis of SM by sphingomyelinase were compared for membranes prepared from 5:5:1 DOPC/sphingomyelin/cholesterol mixtures. Both methods of ceramide incorporation resulted in enlargement of the initial small ordered domains. However, enzymatic ceramide generation led to a much more pronounced restructuring of the bilayer to give large clusters of domains with adjacent areas of a lower phase. The individual domains were heterogeneous with two distinct heights, the highest of which is assigned to a ceramide-rich phase which is hypothesized to occur via ceramide flip-flop to the lower leaflet with formation of a raised domain due to negative membrane curvature. A combination of AFM and fluorescence showed that the bilayer restructuring starts rapidly after enzyme addition, with formation of large clusters of domains at sites of high enzyme activity. The clustering of domains is accompanied by redistribution of fluid phase to the periphery of the domain clusters and there is a continued slow evolution of the bilayer over a period of an hour or more after the enzyme is removed. The relevance of the observed clustering of small nanoscale domains to the postulated coalescence of raft domains to form large signaling platforms is discussed.     

Identification of P2X2/P2X4/P2X6 heterotrimeric receptors using atomic force microscopy (AFM) imaging

Seven P2X purinergic receptor subunits have been identified: P2X1–P2X7. The overlapping expression of P2X2, P2X4 and P2X6 subunits has been shown in different cell types, and functional analysis of P2X receptors in Leydig cells suggests that the three subunits might interact. Here, His₆-tagged P2X2, HA-tagged P2X4 and FLAG-tagged P2X6 subunits were co-expressed in tsA 201 cells. After sequential co-immunoprecipitation using anti-HA and anti-FLAG beads, all three subunits were present, demonstrating their interaction. Atomic force microscopy (AFM) imaging revealed receptors that were specifically decorated by both an anti-His₆ antibody and an anti-HA Fab fragment, indicating the presence of a P2X2/4/6 heterotrimer. To our knowledge, this is the first report of a P2X receptor containing three different subunits.     

Molecular resolution visualization of a pore formed by trichogin,an antimicrobial peptide,in a phospholipid matrix

Electrochemical scanning tunneling microscopy (EC-STM) was employed to study the aggregation of trichogin OMe (TCG), an antimicrobial peptide, incorporated into a lipid monolayer. High-resolution EC-STM images show that trichogin molecules aggregate to form channels in the lipid monolayer. Two types of aggregates were observed in the images. The first consisted of a bundle of six TCG molecules surrounding a central pore. The structure and dimensions of this channel are similar to aggregates that in bilayers are described by the barrel-stave model. The EC-STM images also reveal that channels aggregate further to form a hexagonal lattice of a two dimensional (2D) nanocrystal. The model of 2D lattice was built from trimers of TCG molecules that alternatingly are oriented with either hydrophilic or hydrophobic faces to each other. In this way each TCG molecule is oriented partially with its hydrophilic face towards the hexameric pore allowing the formation of the column of water inside this pore.     

Ultrastable atomic force microscopy: Improved force and positional stability

Atomic force microscopy (AFM) is an exciting technique for biophysical studies of single molecules, but its usefulness is limited by instrumental drift. We dramatically reduced positional drift by adding two lasers to track and thereby actively stabilize the tip and the surface. These lasers also enabled label-free optical images that were spatially aligned to the tip position. Finally, sub-pN force stability over 100 s was achieved by removing the gold coating from soft cantilevers. These enhancements to AFM instrumentation can immediately benefit research in biophysics and nanoscience.     

Ascorbyl palmitate interaction with phospholipid monolayers: Electrostatic and rheological preponderancy

Ascorbyl palmitate (ASC₁₆) is an anionic amphiphilic molecule of pharmacological interest due to its antioxidant properties. We found that ASC₁₆ strongly interacted with model membranes. ASC₁₆ penetrated phospholipid monolayers, with a cutoff near the theoretical surface pressure limit. The presence of a lipid film at the interface favored ASC₁₆ insertion compared with a bare air/water surface. The adsorption and penetration time curves showed a biphasic behavior: the first rapid peak evidenced a fast adsorption of charged ASC₁₆ molecules to the interface that promoted a lowering of surface pH, thus partially neutralizing and compacting the film. The second rise represented an approach to the equilibrium between the ASC₁₆ molecules in the subphase and the surface monolayer, whose kinetics depended on the ionization state of the film. Based on the Langmuir dimiristoylphosphatidylcholine + ASC₁₆ monolayer data, we estimated an ASC₁₆ partition coefficient to dimiristoylphosphatidylcholine monolayers of 1.5 × 10⁵ and a ΔG_p = − 6.7 kcal·mol^− 1. The rheological properties of the host membrane were determinant for ASC₁₆ penetration kinetics: a fluid membrane, as provided by cholesterol, disrupted the liquid-condensed ASC₁₆-enriched domains and favored ASC₁₆ penetration. Subphase pH conditions affected ASC₁₆ aggregation in bulk: the smaller structures at acidic pHs showed a faster equilibrium with the surface film than large lamellar ones. Our results revealed that the ASC₁₆ interaction with model membranes has a highly complex regulation. The polymorphism in the ASC₁₆ bulk aggregation added complexity to the equilibrium between the surface and subphase form of ASC₁₆, whose understanding may shed light on the pharmacological function of this drug.     

Three-dimensional structure of the transmembrane domain of Vpu from HIV-1 in aligned phospholipid bicelles

The three-dimensional backbone structure of the transmembrane domain of Vpu from HIV-1 was determined by solid-state NMR spectroscopy in two magnetically-aligned phospholipid bilayer environments (bicelles) that differed in their hydrophobic thickness. Isotopically labeled samples of Vpu(2-30+), a 36-residue polypeptide containing residues 2-30 from the N-terminus of Vpu, were incorporated into large (q = 3.2 or 3.0) phospholipid bicelles composed of long-chain ether-linked lipids (14-O-PC or 16-O-PC) and short-chain lipids (6-O-PC). The protein-containing bicelles are aligned in the static magnetic field of the NMR spectrometer. Wheel-like patterns of resonances characteristic of tilted transmembrane helices were observed in two-dimensional (1)H/(15)N PISEMA spectra of uniformly (15)N-labeled Vpu(2-30+) obtained on bicelle samples with their bilayer normals aligned perpendicular or parallel to the direction of the magnetic field. The NMR experiments were performed at a (1)H resonance frequency of 900 MHz, and this resulted in improved data compared to lower-resonance frequencies. Analysis of the polarity-index slant-angle wheels and dipolar waves demonstrates the presence of a transmembrane alpha-helix spanning residues 8-25 in both 14-O-PC and 16-O-PC bicelles, which is consistent with results obtained previously in micelles by solution NMR and mechanically aligned lipid bilayers by solid-state NMR. The three-dimensional backbone structures were obtained by structural fitting to the orientation-dependent (15)N chemical shift and (1)H-(15)N dipolar coupling frequencies. Tilt angles of 30 degrees and 21 degrees are observed in 14-O-PC and 16-O-PC bicelles, respectively, which are consistent with the values previously determined for the same polypeptide in mechanically-aligned DMPC and DOPC bilayers. The difference in tilt angle in C14 and C16 bilayer environments is also consistent with previous results indicating that the transmembrane helix of Vpu responds to hydrophobic mismatch by changing its tilt angle. The kink found in the middle of the helix in the longer-chain C18 bilayers aligned on glass plates was not found in either of these shorter-chain (C14 or C16) bilayers.     

Specific anchoring modes of two distinct dystrophin rod sub-domains interacting in phospholipid Langmuir films studied by atomic force microscopy and PM-IRRAS

Dystrophin rod repeats 1-3 sub-domain binds to acidic phosphatidylserine in a small vesicle binding assay, while the repeats 20-24 sub-domain does not. In the present work, we studied the adsorption behaviour of both sub-domains at the air/liquid interface and at the air/lipid interface in a Langmuir trough in order to highlight differences in interfacial properties. The adsorption behaviour of the two proteins at the air/liquid interface shows that they display surface activity while maintaining their alpha-helical secondary structure as shown by PM-IRRAS. Strikingly, R20-24 needs to be highly hydrated even at the interface, while this is not the case for R1-3, indicating that the surface activity is dramatically higher for R1-3 than R20-24. Surface-pressure measurements, atomic force microscopy and PM-IRRAS are used in a Langmuir experiment with DOPC-DOPS monolayers at two different surface pressures, 20 mN/m and 30 mN/m. At the lower surface pressure, the proteins are adsorbed at the lipid film interface while maintaining its alpha-helical structure. After an increase of the surface pressure, R1-3 subsequently produces a stable film, while R20-24 induces a reorganization of the lipid film with a subsequent decrease of the surface pressure close to the initial value. AFM and PM-IRRAS show that R1-3 is present in high amounts at the interface, being arranged in clusters representing 3.3% of the surface at low pressure. By contrast, R20-24 is present at the interface in small amounts bound only by a few electrostatic residues to the lipid film while the major part of the molecule remains floating in the sub-phase. Then for R1-3, the electrostatic interaction between the proteins and the film is enhanced by hydrophobic interactions. At higher surface pressure, the number of protein clusters increases and becomes closer in both cases implying the electrostatic character of the binding. These results indicate that even if the repeats exhibit large structural similarities, their interfacial properties are highly contrasted by their differential anchor mode in the membrane. Our work provides strong support for distinct physiological roles for the spectrin-like repeats and may partly explain the effects of therapeutic replacement of dystrophin deficiency by minidystrophins.