Les biofilms sont des communautés de microorganismes incorporés dans une matrice exo-polymérique complexe. Ils sont reconnus pour jouer un rôle important comme barrière de diffusion dans les systèmes environnementaux et la santé humaine, donnant lieu à une résistance accrue aux antibiotiques et aux désinfectants. Comme le transfert de masse dans un biofilm est principalement dû à la diffusion moléculaire, il est primordial de comprendre les principaux paramètres influençant les flux de diffusion. Dans ce travail, nous avons étudié un biofilm de Pseudomonas fluorescens et deux hydrogels modèles (agarose et alginate) pour lesquels l’autodiffusion (mouvement Brownien) et les coefficients de diffusion mutuels ont été quantifiés. La spectroscopie par corrélation de fluorescence a été utilisée pour mesurer les coefficients d'autodiffusion dans une volume confocal de ca. 1 m3 dans les gels ou les biofilms, tandis que les mesures de diffusion mutuelle ont été faites par cellule de diffusion. En outre, la voltamétrie sur microélectrode a été utilisée pour évaluer le potentiel de Donnan des gels afin de déterminer son impact sur la diffusion. Pour l'hydrogel d'agarose, les observations combinées d'une diminution du coefficient d’autodiffusion et de l’augmentation de la diffusion mutuelle pour une force ionique décroissante ont été attribuées au potentiel de Donnan du gel. Des mesures de l'effet Donnan (différence de -30 mV entre des forces ioniques de 10-4 et 10-1 M) et l'accumulation correspondante d’ions dans l'hydrogel (augmentation d’un facteur de 13 par rapport à la solution) ont indiqué que les interactions électrostatiques peuvent fortement influencer le flux de diffusion de cations, même dans un hydrogel faiblement chargé tel que l'agarose. Curieusement, pour un gel plus chargé comme l'alginate de calcium, la variation de la force ionique et du pH n'a donné lieu qu'à de légères variations de la diffusion de sondes chargées dans l'hydrogel. Ces résultats suggèrent qu’en influençant la diffusion du soluté, l'effet direct des cations sur la structure du gel (compression et/ou gonflement induits) était beaucoup plus efficace que l'effet Donnan. De même, pour un biofilm bactérien, les coefficients d'autodiffusion étaient pratiquement constants sur toute une gamme de force ionique (10-4-10-1 M), aussi bien pour des petits solutés chargés négativement ou positivement (le rapport du coefficient d’autodiffusion dans biofilm sur celui dans la solution, Db/Dw ≈ 85 %) que pour des nanoparticules (Db/Dw≈ 50 %), suggérant que l'effet d'obstruction des biofilms l’emporte sur l'effet de charge. Les résultats de cette étude ont montré que parmi les divers facteurs majeurs qui affectent la diffusion dans un biofilm environnemental oligotrophe (exclusion stérique, interactions électrostatiques et hydrophobes), les effets d'obstruction semblent être les plus importants lorsque l'on tente de comprendre la diffusion du soluté. Alors que les effets de charge ne semblaient pas être importants pour l'autodiffusion de substrats chargés dans l'hydrogel d'alginate ou dans le biofilm bactérien, ils ont joué un rôle clé dans la compréhension de la diffusion à travers l’agarose. L’ensemble de ces résultats devraient être très utiles pour l'évaluation de la biodisponibilité des contaminants traces et des nanoparticules dans l'environnement. / Biofilms are primarily communities of microorganisms embedded in a complex exopolymer matrix. They are thought to play an important role as diffusive barriers in environmental systems and human health, resulting in increased resistance to disinfectants and antibiotics. Since mass transport in a biofilm is primarily due to molecular diffusion, it is critical to understand the main parameters influencing diffusive fluxes in a biofilm. In this thesis, a Pseudomonas fluorescens biofilm and two model hydrogels, (agarose and calcium alginate), were investigated. Both self-diffusion (Brownian motion) and mutual diffusion coefficients were quantified. Fluorescence correlation spectroscopy was used to measure the self-diffusion coefficients in a ca. 1 m3 confocal volume in the gels or biofilms, whereas a diffusion cell setup was employed for mutual diffusion measurements. In addition, microelectrode voltammetry was used to evaluate Donnan potential of the gels in order to determine its impact on diffusion. For the agarose hydrogel, the combined observations of a decreasing self-diffusion coefficient coupled with increasing mutual diffusion as a function of a decreasing ionic strength have been attributed to the gel’s Donnan potential. Measurements of the Donnan effect (difference of -30 mV between ionic strengths of 10-4 and 10-1 M) and the corresponding accumulation of ions in the hydrogel (13x enhancement with respect to the bulk solution) indicated that electrostatic interactions can strongly influence the diffusive flux of cations, even in a weakly charged hydrogel, such as agarose. Somewhat surprisingly, for a more highly charged gel such as calcium alginate, varying ionic strength and pH resulted in only small changes to the diffusion of charged probes in the hydrogel. These results suggested that the direct effect of the cations on gel structure (due to an induced swelling or compression) was much more effective than the Donnan effect when influencing solute diffusion. Similarly, for a bacterial biofilm, self-diffusion coefficients were virtually constant across a range of examined ionic strengths (10-4-10-1 M) for both negatively and positively charged small solutes (Db/Dw≈85%) and nanoparticles (Db/Dw≈50%), suggesting that the obstruction effect of the biofilms again overwhelmed the charge effect. The results of this work indicated that among the various major factors affecting diffusion in an oligotrophic environmental biofilm (steric exclusion, hydrophobic and electrostatic interactions), obstruction effects appeared to be the most important when attempting to understand the solute diffusion. While charge effects did not appear to be important to the self-diffusion of charged substrates in the alginate hydrogel or bacterial biofilm, they were key to understanding diffusion through another gel, with numerous biomedical and environmental applications, i.e. agarose. These results should be extremely useful when evaluating the bioavailability of the trace contaminants and nanoparticles in the environment.

No description available.

Tato práce se zabývá studiem fluorescenčně značeného hyaluronanu, konkrétně rhodaminylamino hyaluronátu sodného (Hya-Rh, 40 kDa), pomocí dvouohniskové fluorescenční korelační spektroskopie (2f-FCS). Nejdříve byla prostudována literatura týkající se využití FCS techniky v koloidní chemii a při studiu polymerů, přičemž následně byly shrnuty veškeré poznatky o využití 2f-FCS metody. Na základě prvotních měření byl zjištěn vhodný postup přípravy a způsob uchovávání vzorku Hya-Rh používaném pro následující experimenty. Záhy byly prostudovány možné vlivy koncentrace Hya-Rh na jeho difúzní charakteristiky jak ve vodě, tak ve fyziologickém roztoku. Následně bylo studováno chování Hya-Rh a vliv koncentrace solí alkalických kovů ve vodných roztocích těchto solí a fluorescenčně značeného hyaluronanu. Poté bylo sledováno chování Hya-Rh v závislosti na koncentraci velmi nízkomolekulárního hyaluronanu (VLMW HA, 404 kDa) v čisté vodě i ve fyziologickém roztoku, přičemž získané výsledky byly mezi sebou porovnány. Nakonec bylo využití 2f-FCS metody celkově zhodnoceno a popsáno z hlediska studia chování fluorescenčně značeného hyaluronanu v roztocích.

The coiled-coil motif is present in proteins from all kingdoms of life. Its structure is based on a repeating sequence of 7 amino acids with hydrophobic residues at positions 1 and 4, which folds into an alpha-helix. Two, or more, alpha-helices wind around each other based on hydrophobic interactions forming the coiled-coil. Structural variations include length, deviations from the canonical form based on the heptad repeat, as well as the orientation and number of alpha-helices. They are involved in a wide variety of cellular processes including vesicle tethering and signal transmission along their length. In order to transmit signal, the protein must be able to dynamically rearrange its structure. An outstanding example of a coiled-coil that needs to rearrange its structure to perform its function is the early endosomal tether EEA1, which has been shown to increase its flexibility upon binding to the active form of the small GTPase Rab5. That conformational change generates an entropic collapse that brings the ends of the protein closer to each other. Nevertheless, the recycling from the more flexible state to its original extended conformation was not addressed. Herein, the entropic collapse mechanism was further studied and the full EEA1 cycle between extended and flexible states described. In addition to these studies, other coiled-coil proteins were assessed to determine if they also experience a binding-induced entropic collapse. One of the strategies to investigate the entropic collapse mechanism was to compare the adhesive forces along the two alpha-helices of the EEA1 dimer in its extended and flexible conformations. To this end, an experiment was designed to unwind the dimer using optical tweezers, a force-spectroscopy method that uses a highly focused laser beam to manipulate microscopic objects. Each EEA1 monomer was attached to a distinct DNA piece using a site-specific enzymatic reaction. The DNA pieces were linked to two optically trapped micron-sized beads. And the distance between the optical traps increased to unwind the EEA1. A second strategy to investigate the entropic collapse was to evaluate EEA1 dynamics in solution using dual color fluorescence cross-correlation spectroscopy (dcFCCS). EEA1 C-termini was labeled with two different fluorophores. Fluctuations on fluorescent intensities caused by the dyes crossing a confocal volume were recorded over time. Based on an analysis of these fluctuations, a conformational change in EEA1 from semi-flexible to flexible upon addition of active Rab5 was described. This is in agreement with the previously reported entropic collapse. More importantly, EEA1 was shown to cycle between semi-flexible and flexible states by adding Rab5:GTP and waiting for the GTP to hydrolyse. To determine whether other proteins experience a binding-induced entropic collapse, coiled-coil proteins that share structural and functional similarities with EEA1 were evaluated. Rotary shadowing EM images of the target protein alone and binding with its suspected allosteric effector were compared. It was found that ELKS, a coiled-coil protein involved in vesicle trafficking, undergoes an increase in flexibility upon binding with the active form of Rab6. Thus, hinting that the entropic collapse may indeed be a general mode of action for at least a sub-group of long coiled-coil proteins. Overall, the major contributions of this thesis are to describe the full entropic collapse cycle on EEA1 and to show a second example of a coiled-coil protein experiencing a binding induced flexibility increase.:List of Figures List of Tables List of Equations List of Abbreviations 1 Introduction 1.1 EEA1 as an endosomal tether 2 Materials and Methods 2.1 Materials 2.2 Methods 2.2.1 Sub-cloning 2.2.2 Protein expression and purification 2.2.3 Protein-protein binding assays 2.2.4 Electron microscopy 2.2.5 Analysis of electron microscopy 2.2.6 Generation of DNA handles for protein-DNA conjugates 2.2.7 Adding SortaseA recognition site to EEA1 2.2.8 Protein-DNA conjugation3 2.2.9 Sample preparation for optical tweezers 2.2.10 Dual color labeling of EEA1 2.2.11 Fluorescence cross-correlation spectroscopy 2.2.12 Generation of dsDNA for dcFCCS calibration 2.2.13 RabGTPase nucleotide loading 2.2.14 Liposome preparation 2.2.15 MCBs preparation 3 Unwinding EEA1 coiled-coil domain 3.1 Introduction 3.1.1 Optical tweezers for EEA1 unwinding 3.1.2 SortaseA-catalysed ligation 3.2 Aims 3.3 Results 3.3.1 Optimization of SortaseA-catalysed ligation 3.3.2 Formation of EEA1-DNA handle conjugate 3.3.3 EEA1 unwinding experiments 3.4 Discussion 4 EEA1 entropic collapse is recyclable 4.1 Introduction 4.1.1 Advantages of dcFCCS vs FCS 4.1.2 Requirements for dcFCCS measurements 4.1.3 dcFCCS for end polymer dynamics analysis 4.2 Aims 4.3 Results 4.3.1 System preparation and dcFCCS calibration 4.3.2 Labelling of EEA1 4.3.3 Comparing FCS vs dcFCCS 4.3.4 EEA1 entropic collapse shown by dcFCCS 4.3.5 EEA1 flexibility change is recyclable 4.4 Discussion 5 Entropic collapse as a general mechanism 5.1 Introduction 5.2 Aims 5.3 Results 5.3.1 ELKS increases its flexibility upon binding active Rab6 5.3.2 p115-GM130 complex observed by rotary shadowing EM 5.4 Discussion 6 Conclusions and outlook References

No description available.

Endocytosis is one of the most fundamental mechanisms by which the cell communicates with its surrounding. Specific signals are transduced through the cell membrane by a complex interplay between proteins and lipids. Clathrin depended endocytosis is one of important signalling pathways which leads to budding of the plasmalemma and a formation of endosomes. The FCHo2 is an essential protein at the initial stage of the this process. In is a membrane binding protein containing BAR (BIN, Amphiphysin, Rvs) domain which is responsible for a membrane binding. Although numerous valuable work on BAR proteins was published recently, the mechanistic description of a BAR domain functionality is missing. In present work we applied in vitro systems in order to gain knowledge about molecular basis of the activity of the FCHo2 BAR domain. In our studies we used supported lipid bilayers (SLBs) and lipid monolayers as s model membrane system. The experiments were carried out with a minimal number of components including the purified FCHo2 BAR domain. Using SLBs we showed that the BAR domain can bind to entirely flat bilayers. We also demonstrated that these interactions depend on the negatively charged lipid species incorporated in the membrane. We designed an assay which allows to quantify the membrane tubulation. We found out that the interaction of the FCHo2 BAR domain with the lipid membrane is concentration dependent. We showed that an area of the bilayer deformed by the protein depends on the amount of the used BAR domain. In order to study the relation between the mobility of lipids and the activity of FCHo2 BAR domain we designed a small-volume monolayer trough. The design of this micro-chamber allows for the implementation of the light microscopy. We demonstrated that the measured lipid diffusion in the monolayer by our new approach is in agreement with literature data. We carried out fluorescence correlation spectroscopy (FCS) experiments at different density of lipids at the water-air interface.We showed that the FCHo2 BAR domain binding affinity is proportional to the mean molecular area (MMA). We additionally demonstrated that the increased protein binding is correlated with the higher lipid mobility in the monolayer. Additionally, by curing out high-speed atomic force microscopy (hsAFM) we acquired the structural information about FCHo2 BAR domains orientation at the membrane with a high spatio-temporal resolution. Obtained data indicate the BAR domains interact witheach other by many different contact sites what results in a variety of protein orientations in a protein assemble.

The goal of this project is to study novel nanoscale excitation volumes, sensitive enoughto study individual chromophores and go on to study new and exciting self assemblyapproaches to this problem. Small excitation volumes may be engineered using light con-finement inside apertures in metal films. These apertures enhance fluorescence emissionrates, quantum yields, decrease fluorescence quenching, enable higher signal-to-noiseratios and allow higher concentration single chromophore fluorescence, to be studied byrestricting this excitation volume. Excitation volumes are reported on using the chro-mophore's fluorescence by utilising fluorescence correlation spectroscopy, which monitorsfluctuations in fluorescence intensity. From the correlation in time, we can find the res-idence time, the number of chromophores, the volume in which they are diffusing andtherefore the fluorescence emission efficiency. Fluorescence properties are a probe ofthe local environment, a particularly powerful tool due to the high brightness (quantumyield) fluorescent dyes and sensitive photo-detection equipment both of which are readilyavailable, (such as avalanche photodiodes and photomultiplier tubes). Novel materialscombining the properties of conducting and non-conducting materials at scales muchsmaller than the incident wavelength are known as meta-materials. These allow combi-nations of properties not usually possible in natural materials at optical frequencies. Theproperties reported so far include; negative refraction, negative phase velocity, fluorescenceemission enhancement, lensing and therefore light confinement has also been proposed tobe possible. Instead of expensive and slow lithography methods many of these materialsmay be fabricated with self assembly techniques, which are truly nanoscopic and otherwiseinaccessible with even the most sophisticated equipment. It was found that nanoscaled volumes from ZMW and HMMs based on NW arrays wereall inefficient at enhancing fluorescence. The primary cause was the reduced fluorescencelifetime reducing the fluorescence efficiency, which runs contrary to some commentatorsin the literature. NW based lensing was found to possible in the blue region of the opticalspectrum in a HMM, without the background fluorescence normally associated with a PAAtemplate. This was achieved using a pseudo-ordered array of relatively large nanowireswith a period just smaller than lambda / 2 which minimised losses. Nanowires in the traditionalregime lambda / 10 produced significant scattering and lead to diffraction, such that they werewholly unsuitable for an optical lensing application.

The subject of this thesis is the generation of spatial temporal structures in living cells. Specifically, we studied the Min-system in the bacterium Escherichia coli. It consists of the MinC, the MinD, and the MinE proteins, which play an important role in the correct selection of the cell division site. The Min-proteins oscillate between the two cell poles and thereby prevent division at these locations. In this way, E. coli divides at the center, producing two daughter cells of equal size, providing them with the complete genetic patrimony. Our goal is to perform a quantitative study, both theoretical and experimental, in order to reveal the mechanism underlying the Min-oscillations. Experimentally, we characterize theMin-system, measuring the temporal period of the oscillations as a function of the cell length, the time-averaged protein distributions, and the in vivo Min-protein mobility by means of different fluorescence microscopy techniques. Theoretically, we discuss a deterministic description based on the exchange of Minproteins between the cytoplasm and the cytoplasmic membrane and on the aggregation current induced by the interaction between membrane-bound proteins. Oscillatory solutions appear via a dynamic instability of the homogenous protein distributions. Moreover, we perform stochastic simulations based on a microscopic description, whereby the probability for each event is calculated according to the corresponding probability in the master equation. Starting from this microscopic description, we derive Langevin equations for the fluctuating protein densities which correspond to the deterministic equations in the limit of vanishing noise. Stochastic simulations justify this deterministic model, showing that oscillations are resistant to the perturbations induced by the stochastic reactions and diffusion. Predictions and assumptions of our theoretical model are compatible with our experimental findings. Altogether, these results enable us to propose further experiments in order to quantitatively compare the different models proposed so far and to test our model with even higher precision. They also point to the necessity of performing such an analysis through single cell measurements.

No description available.

No description available.