A series of sulfonate anionic lipids esters derived from 4-sulfobenzoic acid (single chain) or 5-sulfoisophthalic acid (double chain) with chain length from C14 to C18 were synthesized and characterized. The sodium salts were uniformly insoluble in ethanol; the tetramethylammonium salts of the single chain derivative from oleyl alcohol and the double chain derivative from 2-octyldodecan-1-ol were sufficiently soluble for subsequent experiments. Lipids in ethanol and aqueous buffers were mixed in a microfluidic system (NanoAssmblr ® microfluidic mixer) to prepare a lipid dispersion containing vesicles and/or nanoparticles. Initial studies on prediction and controlling vesicle size based on lipid geometric parameters showed that particle size could be successfully affected and controlled by altering lipid compositions consistent with the formation of vesicles. A survey using high resolution cryo-Scanning Transmission Electron microscopy of the sample made by the microfluidic mixer demonstrated that vesicles were formed but a majority of the sample reformed to other aggregates, which complicated the interpretation of the initial product distribution. Further investigation on the efficiency of incorporation of phospholipids into vesicles indicated that 55% of the initial phospholipid appeared in the vesicle fractions. Sulfonate anionic lipids are incorporated into vesicles with lower efficiency and reach a threshold beyond which the sulfonate lipid is not incorporated. Entrapment efficiency was studied with three dyes. Different concentrations of the hydrophobic neutral dye Nile red, the hydrophilic cationic dye neutral red and the hydrophilic anionic dye hydroxypyrene trisulfonate (HPTS) were prepared. The entrapment efficiency was quantitatively analyzed by HPLC, and electrospray mass spectrometry; up to 15% of the initial dye present could be entrapped. Vesicles permeability assays using the ion channel gramicidin and the ion carrier valinomycin with HPTS-loaded vesicle samples showed that vesicle samples made by the microfluidic mixer and made by a conventional extrusion method appeared to behave in the same manner. Addition of a sulfonate anionic lipid to the lipid mixture resulted in vesicle leakage. The unilamellar proportion of HPTS loaded vesicle samples was assessed using a mellitin assay. A vesicle sample made by the microfluidic mixer was 80% unilamellar; a vesicle sample made by the extrusion method on the same lipid mixture was 60% unilamellar. / Graduate / mengxiuzheng@gmail.com

É conhecido que a força iônica do meio desempenha um papel fundamental na estrutura de vesículas aniônicas de DMPG (dimiristoil fosfatidilglicerol) em dispersões aquosas. A baixa força iônica (~ 6 mM), as dispersões de DMPG exibem várias características anômalas, que foram interpretadas como a abertura de poros na bicamada ao longo da larga região de transição de fase gel-fluida (de ~ 18°C a 30°C). Aqui, revisitamos o sistema de DMPG em tampão a baixa força iônica, mas com dispersões obtidas após a extrusão por filtros de 100 nm, portanto menos polidispersas. Para enfatizar as interações eletrostáticas entre as cabeças polares dos lipídios, que não estarão blindadas pela presença de sais na solução, estudamos dispersões de DMPG em água pura, de modo a monitorar os agregados presentes na dispersão, e suas interações. As dispersões em água foram caracterizadas antes e depois da extrusão. Para tal, utilizamos diversas técnicas experimentais, em diferentes temperaturas: espalhamento de luz estático (SLS) e dinâmico (DLS), calorimetria diferencial de varredura (DSC), Ressonância Paramagnética Eletrônica (RPE) de marcadores de spin incorporados aos agregados, espalhamento de raios-X a altos e baixos ângulos (WAXS e SAXS), e medidas de viscosidade, turbidez, mobilidade eletroforética e condutividade elétrica. Resultados das várias técnicas com dispersões extrusadas de DMPG em tampão mostraram que o comportamento anômalo é observado de forma similar ao de dispersões não extrusadas. Entretanto, o pico de SAXS em muito baixo ângulo é visto de 5 a 45°C, e não apenas na região de transição de fase, portanto não deve ser modelado como a distância entre poros na bicamada lipídica que se abririam nesta região. A distância de repetição relacionada a este pico diminui na região de transição de fase, e com o aumento da concentração lipídica. Medidas de DSC indicaram que, em água, a região de transição de fase da vesícula de DMPG é ainda mais ampla, começando em torno de 10°C, mas ainda terminando em ~ 30oC. No entanto, a alta condutividade elétrica, viscosidade, mobilidade eletroforética, raio efetivo, e a baixa turbidez, vistas apenas na região de transição de fase do DMPG em tampão, são encontradas até altas temperaturas em água, quando a bicamada lipídica já se encontra na fase fluida. Medidas de RPE e WAXS mostraram a transição da membrana de uma fase mais rígida/imóvel/organizada para uma fase mais frouxa/móvel. Dados de espalhamento de luz, RPE e SAXS mostram que, similar ao DMPG em tampão, em água, o DMPG organiza-se como vesículas esféricas, unilamelares, mas possivelmente menores e mais carregadas, exibindo fortes interações vesícula-vesícula. Nas medidas de SAXS, o pico de Bragg na região de muito baixo ângulo foi visto em todas as temperaturas (de 5 a 60°C), sendo que a distância de repetição diminui para temperaturas maiores do que 10oC. Os resultados obtidos para dispersões em água, reforçam o comportamento anômalo observado anteriormente para dispersões em tampão em baixa força iônica. De acordo com eles, propomos a existência de vesículas altamente deformadas e ionizadas a partir de uma certa temperatura, T1 para o DMPG em água e Tmon em tampão baixa força iônica, sendo que em água a forte repulsão eletrostática PG--PG- levaria a fortes deformações e interações vesícula-vesícula, em uma ampla extensão de temperaturas. / It is known that the ionic strength plays a fundamental role in the structure of DMPG (dimyristoyl phosphatidylglycerol) anionic vesicles in water medium. At low ionic strength (~ 6 mM), DMPG dispersions display several anomalous characteristics, which were interpreted as the opening of bilayer pores along the wide bilayer gel-fluid transition region (from ~ 18°C to 30°C). Here, we revisit DMPG in buffer at low ionic strength, but with dispersions obtained after the extrusion by 100 nm filters, thus less polydisperse. To emphasize electrostatic interactions between the polar head-groups, which will not be shielded by ions in solution, we studied DMPG dispersions in pure water to monitor the aggregates in the dispersion and their interactions. Water dispersions were characterized before and after extrusion. For such, we used several experimental techniques, at different temperatures: light scattering, both static (SLS) and dynamic (DLS); differential scanning calorimetry (DSC); electron spin resonance (ESR) of spin labels incorporated into the aggregates, Small and Wide Angle X-Ray Scattering (SAXS and WAXS); and viscosity, turbidity, electrophoretic mobility and electrical conductivity measurements. Several techniques with extruded dispersions of DMPG in buffer showed that the anomalous behavior is also observed. However, the SAXS peak at very low angles is seen from 5 to 45°C, and not only in the phase transition region, therefore it should not be modeled as the distance of correlated pores in the lipid bilayer that would open in this region. The repeating distance related to this peak decreases in the phase transition region, and with increasing lipid concentration. DSC indicates that, in water, the bilayer gel-fluid transition is even wider, starting around 10oC but still ending ~ 30oC. However, high electric conductivity, viscosity, electrophoretic mobility, effective radius and low turbidity found only in the gel-fluid transition region for DMPG in buffer, are found at higher temperatures in water, when lipid bilayers are already in the fluid state. ESR and WAXS measurements evidenced the transition of the membrane from a more rigid/immobile/organized phase to a more soft/mobile phase. Light scattering, ESR and SAXS data showed that, similar to DMPG in buffer, in water, DMPG is organized as spherical unillamelar vesicles, but possibly smaller, highly charged, displaying strong vesicle-vesicle interactions. With SAXS the Bragg peak at very low angles was seen at all temperatures (from 5 to 60°C) with the repetition distance decreasing at temperatures higher than 10 ° C. The results obtained for water dispersions reinforce the anomalous behavior previously observed for buffer at low ionic strength dispersions. According to them, we propose the existence of highly deformed and ionized vesicles from a certain temperature, T1 for DMPG in water and Tmon in buffer at low ionic strength. In water the strong PG- - PG- electrostatic repulsion would lead to strong deformations and vesicle-vesicle interactions, over a wide range of temperatures.

É conhecido que a força iônica do meio desempenha um papel fundamental na estrutura de vesículas aniônicas de DMPG (dimiristoil fosfatidilglicerol) em dispersões aquosas. A baixa força iônica (~ 6 mM), as dispersões de DMPG exibem várias características anômalas, que foram interpretadas como a abertura de poros na bicamada ao longo da larga região de transição de fase gel-fluida (de ~ 18°C a 30°C). Aqui, revisitamos o sistema de DMPG em tampão a baixa força iônica, mas com dispersões obtidas após a extrusão por filtros de 100 nm, portanto menos polidispersas. Para enfatizar as interações eletrostáticas entre as cabeças polares dos lipídios, que não estarão blindadas pela presença de sais na solução, estudamos dispersões de DMPG em água pura, de modo a monitorar os agregados presentes na dispersão, e suas interações. As dispersões em água foram caracterizadas antes e depois da extrusão. Para tal, utilizamos diversas técnicas experimentais, em diferentes temperaturas: espalhamento de luz estático (SLS) e dinâmico (DLS), calorimetria diferencial de varredura (DSC), Ressonância Paramagnética Eletrônica (RPE) de marcadores de spin incorporados aos agregados, espalhamento de raios-X a altos e baixos ângulos (WAXS e SAXS), e medidas de viscosidade, turbidez, mobilidade eletroforética e condutividade elétrica. Resultados das várias técnicas com dispersões extrusadas de DMPG em tampão mostraram que o comportamento anômalo é observado de forma similar ao de dispersões não extrusadas. Entretanto, o pico de SAXS em muito baixo ângulo é visto de 5 a 45°C, e não apenas na região de transição de fase, portanto não deve ser modelado como a distância entre poros na bicamada lipídica que se abririam nesta região. A distância de repetição relacionada a este pico diminui na região de transição de fase, e com o aumento da concentração lipídica. Medidas de DSC indicaram que, em água, a região de transição de fase da vesícula de DMPG é ainda mais ampla, começando em torno de 10°C, mas ainda terminando em ~ 30oC. No entanto, a alta condutividade elétrica, viscosidade, mobilidade eletroforética, raio efetivo, e a baixa turbidez, vistas apenas na região de transição de fase do DMPG em tampão, são encontradas até altas temperaturas em água, quando a bicamada lipídica já se encontra na fase fluida. Medidas de RPE e WAXS mostraram a transição da membrana de uma fase mais rígida/imóvel/organizada para uma fase mais frouxa/móvel. Dados de espalhamento de luz, RPE e SAXS mostram que, similar ao DMPG em tampão, em água, o DMPG organiza-se como vesículas esféricas, unilamelares, mas possivelmente menores e mais carregadas, exibindo fortes interações vesícula-vesícula. Nas medidas de SAXS, o pico de Bragg na região de muito baixo ângulo foi visto em todas as temperaturas (de 5 a 60°C), sendo que a distância de repetição diminui para temperaturas maiores do que 10oC. Os resultados obtidos para dispersões em água, reforçam o comportamento anômalo observado anteriormente para dispersões em tampão em baixa força iônica. De acordo com eles, propomos a existência de vesículas altamente deformadas e ionizadas a partir de uma certa temperatura, T1 para o DMPG em água e Tmon em tampão baixa força iônica, sendo que em água a forte repulsão eletrostática PG--PG- levaria a fortes deformações e interações vesícula-vesícula, em uma ampla extensão de temperaturas. / It is known that the ionic strength plays a fundamental role in the structure of DMPG (dimyristoyl phosphatidylglycerol) anionic vesicles in water medium. At low ionic strength (~ 6 mM), DMPG dispersions display several anomalous characteristics, which were interpreted as the opening of bilayer pores along the wide bilayer gel-fluid transition region (from ~ 18°C to 30°C). Here, we revisit DMPG in buffer at low ionic strength, but with dispersions obtained after the extrusion by 100 nm filters, thus less polydisperse. To emphasize electrostatic interactions between the polar head-groups, which will not be shielded by ions in solution, we studied DMPG dispersions in pure water to monitor the aggregates in the dispersion and their interactions. Water dispersions were characterized before and after extrusion. For such, we used several experimental techniques, at different temperatures: light scattering, both static (SLS) and dynamic (DLS); differential scanning calorimetry (DSC); electron spin resonance (ESR) of spin labels incorporated into the aggregates, Small and Wide Angle X-Ray Scattering (SAXS and WAXS); and viscosity, turbidity, electrophoretic mobility and electrical conductivity measurements. Several techniques with extruded dispersions of DMPG in buffer showed that the anomalous behavior is also observed. However, the SAXS peak at very low angles is seen from 5 to 45°C, and not only in the phase transition region, therefore it should not be modeled as the distance of correlated pores in the lipid bilayer that would open in this region. The repeating distance related to this peak decreases in the phase transition region, and with increasing lipid concentration. DSC indicates that, in water, the bilayer gel-fluid transition is even wider, starting around 10oC but still ending ~ 30oC. However, high electric conductivity, viscosity, electrophoretic mobility, effective radius and low turbidity found only in the gel-fluid transition region for DMPG in buffer, are found at higher temperatures in water, when lipid bilayers are already in the fluid state. ESR and WAXS measurements evidenced the transition of the membrane from a more rigid/immobile/organized phase to a more soft/mobile phase. Light scattering, ESR and SAXS data showed that, similar to DMPG in buffer, in water, DMPG is organized as spherical unillamelar vesicles, but possibly smaller, highly charged, displaying strong vesicle-vesicle interactions. With SAXS the Bragg peak at very low angles was seen at all temperatures (from 5 to 60°C) with the repetition distance decreasing at temperatures higher than 10 ° C. The results obtained for water dispersions reinforce the anomalous behavior previously observed for buffer at low ionic strength dispersions. According to them, we propose the existence of highly deformed and ionized vesicles from a certain temperature, T1 for DMPG in water and Tmon in buffer at low ionic strength. In water the strong PG- - PG- electrostatic repulsion would lead to strong deformations and vesicle-vesicle interactions, over a wide range of temperatures.

The interplay between lipids and membrane proteins is known to affect membrane protein topology and thus have significant effect (control) on their functions. In this PhD thesis, the influence of lipids on the membrane protein function was studied using three different membrane protein models. A monotopic membrane protein, monoglucosyldiacylglyecerol synthase (MGS) from Acholeplasma laidlawii is known to induce intracellular vesicles when expressed in Escherichia coli. The mechanism leading to this unusual phenomenon was investigated by various biochemical and biophysical techniques. The results indicated a doubling of lipid synthesis in the cell, which was triggered by the selective binding of MGS to anionic lipids. Multivariate data analysis revealed a good correlation with MGS production. Furthermore, preferential anionic lipid sequestering by MGS was shown to induce a different fatty acid modeling of E. coli membranes. The roles of specific lipid binding and the probable mechanism leading to intracellular vesicle formation were also investigated. As a second model, a MGS homolog from Synechocystis sp. PCC6803 was selected. MgdA is an integral membrane protein with multiple transmembrane helices and a unique membrane topology. The influence of different type of lipids on MgdA activity was tested with different membrane fractions of Synechocystis. Results indicated a very distinct profile compared to Acholeplasma laidlawii MGS. SQDG, an anionic lipid was found to be the species of the membrane that increased the MgdA activity 7-fold whereas two other lipids (PG and PE) had only minor effects on MgdA. Additionally, a working model of MgdA for the biosynthesis and flow of sugar lipids between Synechocystis membranes was proposed. The last model system was another integral membrane protein with a distinct structure but also a different function. The envelope stress sensor, CpxA and its interaction with E. coli membranes were studied. CpxA autophosphorylation activity was found to be positively regulated by phosphatidylethanolamine and negatively by anionic lipids. In contrast, phosphorylation of CpxR by CpxA revealed to be increased with PG but inhibited by CL. Non-bilayer lipids had a negative impact on CpxA phosphotransfer activity. Taken together, these studies provide a better understanding of the significance of the interplay of lipids and model membrane proteins discussed here.

Les cellules eucaryotes possèdent un territoire membranaire dit « électrostatique » qui est définit par la présence de phospholipides négativement chargés sur la face cytosolique des membranes. Cette propriété permet le recrutement de protéine cytosolique contenant des motifs/domaines positivement chargés au niveau des membranes via des interactions électrostatiques. Nous nous sommes demandés si le territoire électrostatique est présent chez les cellules végétales et quel est son organisation ? Quels sont le(s) lipide(s) anionique(s) impliqués dans son maintien ? Et quel est son (ces) rôle(s) dans la signalisation et le développement des plantes ? Premièrement, nous avons mis en avant que la membrane plasmique est le compartiment intracellulaire le plus électronégativement chargé (Simon, Platre et al., 2016 Nature Plants). Ce champ électrostatique est gouverné par trois lipides anioniques différents, l’acide phosphatidique, la phosphatidylserine et le phosphatidylinositol-4-phosphate. Nous avons montré que cette propriété unique de la membrane plasmique permet de réguler des voies de signalisation hormonale, tel que celle de l’auxine et des brassinostéroïdes. Notamment, la phosphatidylserine régule la dynamique spatiotemporelle des petites GTPases de la famille Rho. En réponse à l’auxine, ce lipide permet de regrouper les protéines Rho dans des domaines membranaires. La formation de ces domaines est requise pour l’activité de ces protéines permettant de contrôler l’endocytose, la dynamique du cytosquelette mais également régule la morphogenèse cellulaire ainsi que la réponse gravitropique de la racine. / The « electrostatic territory» is part of the eukaryotic membrane organization and is defined by the enrichment of negatively charged phospholipids at the membrane cytosolic face. This feature is involved in the membrane recruitment of cytosolic proteins, which contain positively charged motifs and/or domains. In this work, we used Arabidopsis thaliana as a model and explored the existence of an electrostatic territory in plant cells. We found that the plasma membrane is the most anionic intracellular membrane (Simon, Platre et al., 2016 Nature Plants). This electrostatic field is maintained by lipid cooperation between, phosphatidic acid, phosphatidylserine and phosphatidylinositol-4-phosphate. The cell surface unique feature is involved in the regulation of hormonal signalling such as auxin and brassinosteroids pathways. We found that phosphatidylserine tunes the spatiotemporal dynamics of small GTPases from the Rho family. During auxin response, PS is required to cluster Rho into specialized membrane domains. We show that nanocluster formation is required for Rho-mediated auxin signaling including the regulation of endocytosis, cytoskeleton organization, morphogenesis and the root gravitropic response.