). The structures of cdMGD1 and cdMGD1:UDP have been deposited in the Protein Data Bank under accession numbers 4WYI and 4X1T, respectively. SUMMARYMonogalactosyldiacylglycerol (MGDG) and digalactosyldiacylglycerol (DGDG) are the major lipid components of photosynthetic membranes, and hence the most abundant lipids in the biosphere. They are essential for assembly and function of the photosynthetic apparatus. In Arabidopsis, the first step of galactolipid synthesis is catalyzed by MGDG synthase 1 (MGD1), which transfers a galactosyl residue from UDP-galactose to diacylglycerol (DAG). MGD1 is a monotopic protein that is embedded in the inner envelope membrane of chloroplasts. Once produced, MGDG is transferred to the outer envelope membrane, where DGDG synthesis occurs, and to thylakoids. Here we present two crystal structures of MGD1: one unliganded and one complexed with UDP. MGD1 has a long and flexible region (approximately 50 amino acids) that is required for DAG binding. The structures reveal critical features of the MGD1 catalytic mechanism and its membrane binding mode, tested on biomimetic Langmuir monolayers, giving insights into chloroplast membrane biogenesis. The structural plasticity of MGD1, ensuring very rapid capture and utilization of DAG, and its interaction with anionic lipids, possibly driving the construction of lipoproteic clusters, are consistent with the role of this enzyme, not only in expansion of the inner envelope membrane, but also in supplying MGDG to the outer envelope and nascent thylakoid membranes.

Dystrophin is essential to skeletal muscle function and confers resistance to the sarcolemma by interacting with cytoskeleton and membrane. In the present work, we characterized the behavior of dystrophin 11-15 (DYS R11-15), five spectrin-like repeats from the central domain of human dystrophin, with lipids. DYS R11-15 displays an amphiphilic character at the liquid/ air interface while maintaining its secondary ␣-helical structure. The interaction of DYS R11-15 with small unilamellar vesicles (SUVs) depends on the lipid nature, which is not the case with large unilamellar vesicles (LUVs). In addition, switching from anionic SUVs to anionic LUVs suggests the lipid packing as a crucial factor for the interaction of protein and lipid. The monolayer model and the modulation of surface pressure aim to mimic the muscle at work (i.e. dynamic changes of muscle membrane during contraction and relaxation) (high and low surface pressure). Strikingly, the lateral pressure modifies the protein organization. Increasing the lateral pressure leads the proteins to be organized in a regular network. Nevertheless, a different protein conformation after its binding to monolayer is revealed by trypsin proteolysis. Label-free quantification by nano-LC/ MS/MS allowed identification of the helices in repeats 12 and 13 involved in the interaction with anionic SUVs. These results, combined with our previous studies, indicate that DYS R11-15 constitutes the only part of dystrophin that interacts with anionic as well as zwitterionic lipids and adapts its interaction and organization depending on lipid packing and lipid nature. We provide strong experimental evidence for a physiological role of the central domain of dystrophin in sarcolemma scaffolding through modulation of lipid-protein interactions.Dystrophin is a rod-shaped cytoplasmic protein that constitutes a vital part of a protein complex that connects the cytoskeleton of muscle fibers to the surrounding extracellular matrix through the cell membrane. This long, filamentous protein (Fig. 1A) is essential to skeletal muscle function, which is demonstrated by the lethal pathophysiology associated with its deficiency, namely Duchenne muscular dystrophy (1). Several membrane and cytoskeletal binding partners of dystrophin have been identified, including ␤-dystroglycan from the dystrophin-glycoprotein complex (2, 3). ␤-Dystroglycan interacts with the cysteine-rich region of dystrophin that is located between the stabilizing central domain, which consists of 24 spectrin-like repeats and is known as the rod domain, and the C-terminal end of the molecule. Cytoskeletal actin interacts with the dystrophin molecule through two actin-binding domains, ABD1 and ABD2, which are situated at the N-terminal end and at the center of the dystrophin rod domain (repeats 11-15), respectively (4). The subsarcolemmal location of dystrophin and its association with both the cytoskeleton and membrane suggest a role in the mechanical regulation of membrane stress during contraction and elongation of muscle fi...

Mono- and digalactosyldiacylglycerol (MGDG and DGDG) are the most abundant lipids of photosynthetic membranes (thylakoids). In Arabidopsis green tissues, MGD1 is the main enzyme synthesizing MGDG. This monotopic enzyme is embedded in the inner envelope membrane of chloroplasts. DGDG synthesis occurs in the outer envelope membrane. Although the suborganellar localization of MGD1 has been determined, it is still not known how the lipid/glycolipid composition influences its binding to the membrane. The existence of a topological relationship between MGD1 and "embryonic" thylakoids is also unknown. To investigate MGD1 membrane binding, we used a Langmuir membrane model allowing the tuning of both lipid composition and packing. Surprisingly, MGD1 presents a high affinity to MGDG, its product, which maintains the enzyme bound to the membrane. This positive feedback is consistent with the low level of diacylglycerol, the substrate of MGD1, in chloroplast membranes. By contrast, MGD1 is excluded from membranes highly enriched in, or made of, pure DGDG. DGDG therefore exerts a retrocontrol, which is effective on the overall synthesis of galactolipids. Previously identified activators, phosphatidic acid and phosphatidylglycerol, also play a role on MGD1 membrane binding via electrostatic interactions, compensating the exclusion triggered by DGDG. The opposite effects of MGDG and DGDG suggest a role of these lipids on the localization of MGD1 in specific domains. Consistently, MGDG induces the self-organization of MGD1 into elongated and reticulated nanostructures scaffolding the chloroplast membrane.-Sarkis, J., Rocha, J., Maniti, O., Jouhet, J., Vié, V., Block, M. A., Breton, C., Maréchal, E., Girard-Egrot, A. The influence of lipids on MGD1 membrane binding highlights novel mechanisms for galactolipid biosynthesis regulation in chloroplasts.

Cell mechanisms are actively modulated by membrane dynamics. We studied the dynamics of a first-stage biomimetic system by Fluorescence Recovery After Patterned Photobleaching. Using this simple biomimetic system, constituted by α -hemolysin from Staphylococcus aureus inserted as single heptameric pore or complexes of pores in a glass-supported DMPC bilayer, we observed true diffusion behavior, with no immobile fraction. We find two situations: i) when incubation is shorter than 15 hours, the protein inserts as a heptameric pore and diffuses roughly three times more slowly than its host lipid bilayer; ii) incubation longer than 15 hours leads to the formation of larger complexes which diffuse more slowly. Our results indicate that, while the Saffman-Delbruck model adequately describes the diffusion coefficient D for small radii, D of the objects decreases as 1/R(2) for the size range explored in this study. Additionally, in the presence of inserted proteins, the gel-to-fluid transition of the supported bilayer as well as a temperature shift in the gel-to-fluid transition are observed.

Biological membranes are highly dynamic in their ability to orchestrate vital mechanisms including cellular protection, organelle compartmentalization, cellular biomechanics, nutrient transport, molecular/enzymatic recognition, and membrane fusion. Controlling lipid composition of different membranes allows cells to regulate their membrane characteristics, thus modifying their physical properties to permit specific protein interactions and drive structural function (membrane deformation facilitates vesicle budding and fusion) and signal transduction. Yet, how lipids control protein structure and function is still poorly understood and needs systematic investigation. In this review, we explore different in vitro membrane models and summarize our current understanding of the interplay between membrane biophysical properties and lipid-protein interaction, taken as example few proteins involved in muscular activity (dystrophin), digestion and Legionella pneumophila effector protein DrrA. The monolayer model with its movable barriers aims to mimic any membrane deformation while surface pressure modulation imitates lipid packing and membrane curvature changes. It is frequently used to investigate peripheral protein binding to the lipid headgroups. Examples of how lipid lateral pressure modifies protein interaction and organization within the membrane are presented using various biophysical techniques. Interestingly, the shear elasticity and surface viscosity of the monolayer will increase upon specific protein(s) binding, supporting the importance of such mechanical link for membrane stability. The lipid bilayer models such as vesicles are not only used to investigate direct protein binding based on the lipid nature, but more importantly to assess how local membrane curvature (vesicles with different size) influence the binding properties of a protein. Also, supported lipid bilayer model has been used widely to characterize diffusion law of lipids within the bilayer and/or protein/biomolecule binding and diffusion on the membrane. These membrane models continue to elucidate important advances regarding the dynamic properties harmonizing lipid-protein interaction.

The K4 peptide (KKKKPLFGLFFGLF) was recently demonstrated to display good antimicrobial activities against various bacterial strains and thus represents a candidate for the treatment of multiple-drug resistant infections. In this study, we use various techniques to study K4 behaviour in different media: water, solutions of detergent micelles, phospholipid monolayers and suspension of phospholipid vesicles. First, self-assembly of the peptide in water is observed, leading to the formation of spherical objects around 10nm in diameter. The addition of micelles induces partial peptide folding to an extent depending on the charge of the detergent headgroups. The NMR structure of the peptide in the presence of SDS displays a helical character of the hydrophobic moiety, whereas only partial folding is observed in DPC micelles. This peptide is able to destabilize the organization of monolayer membranes or bilayer liposomes composed of anionic lipids. When added on small unilamellar vesicles it generates larger objects attributed to mixed lipid-peptide vesicles and aggregated vesicles. The absence of calcein leakage from liposomes, when adding K4, underlines the original mechanism of this linear amphipathic peptide. Our results emphasize the importance of the electrostatic effect for K4 folding and lipid destabilization leading to the microorganisms' death with a high selectivity for the eukaryotic cells at the MIC. Interestingly, the micrographs obtained by electronic microscopy after addition of peptide on bacteria are also consistent with the formation of mixed lipid-peptide objects. Overall, this work supports a detergent-like mechanism for the antimicrobial activity of this peptide.

Dystrophin is an essential part of a membrane protein complex that provides flexible support to muscle fiber membranes. Loss of dystrophin function leads to membrane fragility and muscle-wasting disease. Given the importance of cytoskeletal interactions in strengthening the sarcolemma, we have focused on actin-binding domain 2 of human dystrophin, constituted by repeats 11 to 15 of the central domain (DYS R11-15). We previously showed that DYS R11-15 also interacts with membrane lipids. We investigated the shear elastic constant (μ) and the surface viscosity (η(s)) of Langmuir phospholipid monolayers mimicking the inner leaflet of the sarcolemma in the presence of DYS R11-15 and actin. The initial interaction of 100 nM DYS R11-15 with the monolayers slightly modifies their rheological properties. Injection of 0.125 μM filamentous actin leads to a strong increase of μ and η(s,) from 0 to 5.5 mN/m and 2.4 × 10(-4) N · s/m, respectively. These effects are specific to DYS R11-15, require filamentous actin, and depend on phospholipid nature and lateral surface pressure. These findings suggest that the central domain of dystrophin contributes significantly to the stiffness and the stability of the sarcolemma through its simultaneous interactions with the cytoskeleton and lipid membrane. This mechanical link is likely to be a major contributing factor to the shock absorber function of dystrophin and muscle sarcolemmal integrity on mechanical stress.

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.