Le repliement des protéines est principalement gouverné par les interactions spécifiques des structures secondaires. 1, 2 Toutefois, il existe expérimentalement peu d’informations sur les propriétés mécaniques fondamentales des hélices α et des feuillets β isolées. Les recherches antérieures sur l'étude du déploiement des hélices sont peu concluantes 3-5 et à notre connaissance l'étude des propriétés mécaniques d'un feuillet β isolé, intramoléculaire est sans précédent. Les copolymères PEG114-b-poly(L-lysine)134-(2-pyridyl disulfure),PEG114-b-poly(L-lysine)-b-PEG114 et poly(L-acide glutamique)85-b-(2-pyridyldisulfure) été synthétisés et utilisés comme systèmes modèles pour tester les propriétés mécaniques des motifs secondaires de type hélice α et feuillet β. Les résultats obtenus se sont révélés être en bon accord avec les résultats théoriques obtenus en utilisant un modèle statistique basé sur AGAGIR 6. La différence de force de déroulement comparant les hélices de poly(L-Lysine) ≈ 30 pN et de poly(L-acide glutamique) ≈ 20 pN des copolymères diblocs a été attribuée à l'hydrophobicité différente des chaînes latérales. La plus grande hydrophobie dumotif lysine conduit à de plus grandes interactions entre les chaînes latérales qui empêchent les fluctuations aléatoires au sein de l’hélice, et conduisent à une stabilité supérieure de l'hélice α. Lorsque les expériences ont été conduites dans des conditions favorisant la solubilité des chaînes latérales de lysine, les interactions ont diminué à une force de ≈ 20 pN, similaire à la force des interactions observées pour le poly(L-acide glutamique). Nous supposons qu'un minimum de ≈ 20 pN est nécessaire pour rompre la liaison hydrogène en maintenant l'hélice α, car cette force a été obtenue dans des conditions où les interactions de la chaîne latérale étaient minimisées. La présence de plateaux de force constants et d'inflexions correspondantes démontre une force de dépliement indépendante de la longueur, qui supporte un mécanisme de déroulement tour-par-tour pour l'hélice. De plus, la plus grande hydrophobie des chaînes latérales a été suggérée non seulement pour stabiliser la structure en hélice, mais également pour inhiber la formation d'une structure de type β-turn métastable intermédiaire lorsque les forces entropiques dominent. Des études préliminaires ont été effectuées sur le système de PEG114-bpoly(L-Lysine)134-(2-pyridyl disulfure) après induction d’une transition - β par un traitement thermique dans des conditions basiques. Une inflexion à une force≈ 70 pN a été obtenue, ce qui suggère la formation d'une interaction de type feuillet β. Une stratégie bottom-up a ainsi été proposée avec succès, démontrant le potentiel d'utilisation de tels systèmes artificiels pour simplifier et modéliser des systèmes biologiques réels. La compréhension de ces modèles isolés plus simples aidera sans doute la compréhension de systèmes plus complexes. / Proteins fold by the initial, preferential folding of secondarystructures 1, 2, however surprisingly little is known about the basic mechanicalproperties of isolated α-helices and β-sheets from an experimental standpoint.Previous investigations into studying the generic unfolding behaviour of α-heliceshave proved inconclusive 3-5, and to our knowledge the study of an isolated,intramolecular β-sheet is unprecedented.Bioinspired PEG114-b-poly(L-glutamic acid)85-(2-pyridyl disulphide),PEG114-b-poly(L-lysine)134-(2-pyridyl disulphide) and PEG114-b-poly(Llysine)134–b-PEG114 were designed, synthesized and utilized as model systems toprobe the mechanical properties of α-helix and β-sheet secondary motifs. Theobtained results were shown to be in good agreement with theoretical resultsobtained by utilizing a AGAGIR-based statistical mechanical model 6. Thedifference in unravelling force comparing the helices of poly(L-Lysine) ≈30 pNand poly(L-glutamic acid) ≈20 pN diblock copolymers was attributed to thediffering hydrophobicity of the side chains. The greater hydrophobicity of thelysine allowed greater interactions between the side chains and sterically hinderedrandom helix-coil fluctuations, which lead to a superior α-helix stability. Whenexperiments were conducted in conditions promoting the solubility of the lysineside chains, the interactions decreased to a force of ≈20 pN, similar to the force ofinteractions observed for the poly(L-glutamic acid). We infer that a minimum of≈20 pN is needed to rupture the hydrogen bonding maintaining the α-helix as thisforce was obtained in conditions where the side chain interactions wereminimized.The presence of constant force plateaus and corresponding inflectionsdemonstrates a length independent unfolding force, which supports a turn-by-turnunfolding mechanism for the α-helix.In addition, the greater hydrophobicity of the side chains was suggestedto not only stabilize the α-helix structure, but also to inhibit the formation of anintermediate metastable β-hairpin-like structure when entropic forces dominate.Preliminary studies were also conducted on the PEG114-b-poly(LLysine)134-(2-pyridyl disulphide) system after a α-β transition had been inducedby heat in basic conditions, where an inflection at a much higher force of ≈ 70 pNwas obtained suggesting the formation of a β-sheet interaction.A bottom-up, investigative strategy has thus been successfully proposeddemonstrating the potential of utilizing such artificial systems to simplify andexemplify real biological systems. The comprehension of these simpler isolatedmodels will no doubt aid the understanding of more complex systems.

The Tumor Necrosis Factor derived-TIP peptide is a small 17 amino acids cyclic peptide with lectin-like activity, that possesses several therapeutically relevant biological activities, among which is activation of alveolar liquid clearance in both healthy and injured lungs in vivo. Accumulation of fluid in the lungs? alveoli and interstitial spaces is a life-threatening condition called pulmonary edema. The mortality rate due permeability pulmonary edema, accompanied by a dysfunction of the alveolar/capillary barrier, is high because no effective treatment lacking side effects exists nowadays. It is known that the TIP peptide is able to activate vectorial Na+ transport ? which mediates lung liquid clearance. However, the mechanism of action of remains elusive. The aim of this thesis was to investigate the initial steps of interaction between the TIP peptide and airway epithelial cells. Numerous novel methods and single-molecule techniques were used to unravel: (i) how the TIP peptide interacts with the molecules on the apical side of the lung epithelial cells; (ii) whether the TIP peptide need to be internalized inside of the cells to trigger its effects; (iii) the nature of the interaction between the TIP peptide and its putative receptor(s); (iv) the putative receptor(s) for the TIP peptide on the apical surface of the lung epithelial cells.

L’engouement mondial pour les appareils nomades et la course à la sobriété énergétique font de la diminution de la taille des systèmes microélectroniques (MEMS) un enjeu majeur pour les prochaines années. Les micro batteries au lithium sont aujourd'hui le moyen le plus efficace pour stocker et alimenter des dispositifs avec une très forte densité énergétique. Les incorporer dans des cartes de crédit comportant un écran et des touches intégrés est l’un des défis que relèvent les multinationales comme ST Micro Electronics. Ces micro batteries contiennent cependant du lithium métallique qui peut s'avérer très dangereux quand il est en contact avec de l’eau ou de l’air humide. Ainsi, afin de protéger les composants à une exposition à l’humidité, une encapsulation de l’ensemble de la batterie est nécessaire. L'encapsulation polymère a l’avantage, comparativement à d’autres matériaux, de présenter un faible coût de mise en forme et un faible poids. Cependant, de tels systèmes d'encapsulation sont aujourd'hui insuffisants pour garantir une durée de vie de plusieurs années des composants car en présence d’humidité ou d’une variation de température importante la tenue mécanique des assemblages peut être fragilisée. L'objectif de la thèse est donc de réaliser et d'étudier le comportement mécanique et structural d’assemblage de couches minces de polymères et de métaux en température et en humidité. Deux types de polymères ont été choisis pour ce projet :1. Le chlorure de polyvinylidène (PVDC), un polymère commercial très utilisé pour ses bonnes propriétés barrières à l'eau 2. Un oligomère acrylate reticulable par voie thermique et UV synthétisé au sein de l'IMMM. / The increasing number of mobile devices and the race to energy sobriety make the decrease of the size of microelectronic systems (MEMS) a major challenge. Today, Lithium micro batteries are currently the best solution for high-power-and-energy applications. Incorporate them into credit cards containing a screen or associate them to electronic sensors for the supervision is the challenge which raises international companies such as ST Microelectronics. However, these micro batteries contain some lithium metal which can be dangerous if the metallic lithium is in contact with water or humid air. In addition, the substance can spontaneously ignite in the contact of the humidity. So, in order to avoid the problems of safety, we absolutely have to protect the lithium contained in our micro batteries using an encapsulation layer. Polymeric encapsulation has the advantage, compared with other materials (ceramic, metal), to present a moderate cost of shaping and a low weight. However, such systems of encapsulation are today insufficient to guarantee a satisfactory life cycle of components. Indeed, in the presence of humidity or of a too important temperature variation, the mechanical assemblies can be weakened and engender an irreparable break. The objective of the thesis is therefore to realize and study the mechanical and structural behavior of assembly of thin layers of polymers and metals in temperature and humidity.Two types of polymers were selected for this project:1. Polyvinylidene chloride (PVDC), a commercial polymer widely used for its good barrier properties to water.2. A thermally and UV-crosslinkable acrylate oligomer synthesized in the IMMM.

Die Proteinfaltung ist ein Prozess der molekularen Selbstorganisation, bei dem sich eine lineare Kette von Aminosäuren zu einer definierten, funktionellen dreidimensionalen Struktur zusammensetzt. Der Prozess der Faltung ist ein thermisch getriebener diffusiver Prozess durch eine Gibbs-Energie-Landschaft im Konformationsraum für die Struktur der minimalen Energie. Während dieses Prozesses zeigt die freie Enthalpie des Systems nicht immer eine monotone Abnahme; stattdessen führt eine suboptimale Kompensation der Enthalpie- und der Entropieänderung während jedes Faltungsschrittes zur Bildung von Freien-Enthalpie-Faltungsbarrieren. Diese Barrieren und damit verbundenen hochenergetischen Übergangszustände, die wichtige Informationen über Mechanismen der Proteinfaltung enthalten, sind jedoch kinetisch unzugänglich. Um den Prozess der Barrierebildung und die strukturellen Merkmale von Übergangszuständen aufzudecken, werden Proteine genutzt, die über barrierefreie Pfade falten – so genannte “downhill folder“. Aufgrund der geringen Faltungsbarrieren werden wichtige Interaktionen der Faltung zugänglich und erlauben Einblicke in die ratenbegrenzenden Faltungsvorgänge. In dieser Arbeit vergleichen wir die Faltungsdynamiken von drei verschiedenen Varianten eines Lambda-Repressor-Fragments, bestehend aus den Aminosäuren 6 bis 85: ein Zwei-Zustands-Falter λWT (Y22W) und zwei downhill-folder-artige Varianten, λYA (Y22W/Q33Y/ G46,48A) und λHA (Y22W/Q33H/G46,48A). Um auf die Kinetik und die strukturelle Dynamik zu greifen zu können, werden Einzelmolekülkraftspektroskopische Experimente mit optische Pinzetten mit Submillisekunden- und Nanometer-Auflösung verwendet. Ich fand, dass die niedrige denaturierende Kraft die Mikrosekunden Faltungskinetik von downhill foldern auf eine Millisekunden-Zeitskala verlangsamt, sodass das System für Einzelmolekülstudien gut zugänglich ist. Interessanterweise zeigten sich unter Krafteinwirkung die downhill-folder-artigen Varianten des Lambda-Repressors als kooperative Zwei-Zustands-Falter mit deutlich unterschiedlicher Faltungskinetik und Kraftabhängigkeit. Drei Varianten des Proteins zeigten ein hoch konformes Verhalten unter Last. Die modellfreie Rekonstruktion von Freien-Enthalpie-Landschaften ermöglichte es uns, die feinen Details der Transformation des Zwei-Zustands-Faltungspfad direkt in einen downhill-artigen Pfad aufzulösen. Die Auswirkungen von einzelnen Mutationen auf die Proteinstabilität, Bildung der Übergangszustände und die konformationelle Heterogenität der Faltungs- und Entfaltungszustände konnten beobachtet werden. Interessanterweise zeigen unsere Ergebnisse, dass sich die untersuchten Varianten trotz der ultraschnellen Faltungszeit im Bereich von 2 μs in einem kooperativen Prozess über verbleibende Energiebarrieren falten und entfalten, was darauf hindeutet, dass wesentlich schnellere Faltungsraten notwendig sind um ein downhill Limit vollständig zu erreichen.:I Theoretical background 1 1 Introduction 3 2 Protein folding: the downhill scenario 5 2.1 Protein folding as a diffusion on a multidimensional energy landscape 5 2.2 Downhill folding proteins 7 2.2.1 Thermodynamic description of downhill folders 7 2.2.2 Identification criteria for downhill folders 8 2.3 Lambda repressor as a model system for studying downhill folding 9 2.3.1 Wild-type lambda repressor fragment λ{6-85} 10 2.3.2 Acceleration of λ{6-85} folding by specifific point mutations 11 2.3.3 The incipient-downhill λYA and downhill λHA variants 14 2.4 Single-molecule techniques as a promising tool for probing downhill folding dynamics 17 3 Single-molecule protein folding with optical tweezers 19 3.1 Optical tweezers 19 3.1.1 Working principle of optical tweezers 19 3.1.2 The optical tweezers setup 21 3.2 The dumbbell assay 22 3.3 Measurement protocols 23 3.3.1 Constant-velocity experiments 23 3.3.2 Constant-trap-distance experiments (equilibrium experiments) 24 4 Theory and analysis of single-molecule trajectories 27 4.1 Polymer elasticity models 27 4.2 Equilibrium free energies of protein folding in optical tweezers 28 4.3 Signal-pair correlation analysis 29 4.4 Force dependence of transition rate constants 29 4.4.1 Zero-load extrapolation of rates: the Berkemeier-Schlierf model 30 4.4.2 Detailed balance for unfolding and refolding data 31 4.5 Direct measurement of the energy landscape via deconvolution 32 II Results 33 5 Efficient strategy for protein-DNA hybrid formation 35 5.1 Currently available strategies for protein-DNA hybrid formation 35 5.2 Novel assembly of protein-DNA hybrids based on copper-free click chemistry 37 5.3 Click-chemistry based assembly preserves the native protein structure 40 5.4 Summary 42 6 Non-equilibrium mechanical unfolding and refolding of lambda repressor variants 45 6.1 Non-equilibrium unfolding and refolding of lambda repressor λWT 45 6.2 Non-equilibrium unfolding and refolding of incipient-downhill λYA and downhill λHA variants of lambda repressor 48 6.3 Summary 52 7 Equilibrium unfolding and refolding of lambda repressor variants 53 7.1 Importance of the trap stiffness to resolve low-force nanometer transitions 54 7.2 Signal pair-correlation analysis to achieve millisecond transitions 56 7.3 Force-dependent equilibrium kinetics of λWT 59 7.4 Equilibrium folding of incipient-downhill λYA and downhill λHA variants of lambda repressor 61 7.5 Summary 65 8 Model-free energy landscape reconstruction for λWT, incipient-downhill λYA and downhill λHA variants 69 8.1 Direct observation of the effect of a single mutation on the conformational heterogeneity and protein stability 71 8.2 Artifacts of barrier-height determination during deconvolution 75 8.3 Summary 76 9 Conclusions and Outlook 79 / Protein folding is a process of molecular self-assembly in which a linear chain of amino acids assembles into a defined, functional three-dimensional structure. The process of folding is a thermally driven diffusive search on a free-energy landscape in the conformational space for the minimal-energy structure. During that process, the free energy of the system does not always show a monotonic decrease; instead, sub-optimal compensation of enthalpy and entropy change during each folding step leads to formation of folding free-energy barriers. However, these barriers, and associated high-energy transition states, that contain key information about mechanisms of protein folding, are kinetically inaccessible. To reveal the barrier-formation process and structural characteristics of transition states, proteins are employed that fold via barrierless paths – so-called downhill folders. Due to the low folding barriers, the key folding interactions become accessible, yielding insights about the rate-limiting folding events. Here, I compared the folding dynamics of three different variants of a lambda repressor fragment, containing amino acids 6 to 85: a two-state folder λWT (Y22W) and two downhill-like folding variants, λYA (Y22W/Q33Y/G46,48A) and λHA (Y22W/Q33H/G46,48A). To access the kinetics and structural dynamics, single-molecule optical tweezers with submillisecond and nanometer resolution are used. I found that force perturbation slowed down the microsecond kinetics of downhill folders to a millisecond time-scale, making it accessible to single-molecule studies. Interestingly, under load, the downhill-like variants of lambda repressor appeared as cooperative two-state folders with significantly different folding kinetics and force dependence. The three protein variants displayed a highly compliant behaviour under load. Model-free reconstruction of free-energy landscapes allowed us to directly resolve the fine details of the transformation of the two-state folding path into a downhill-like path. The effect of single mutations on protein stability, transition state formation and conformational heterogeneity of folding and unfolding states was observed. Noteworthy, our results demonstrate, that despite the ultrafast folding time in a range of 2 µs, the studied variants fold and unfold in a cooperative process via residual barriers, suggesting that much faster folding rate constants are required to reach the full-downhill limit.:I Theoretical background 1 1 Introduction 3 2 Protein folding: the downhill scenario 5 2.1 Protein folding as a diffusion on a multidimensional energy landscape 5 2.2 Downhill folding proteins 7 2.2.1 Thermodynamic description of downhill folders 7 2.2.2 Identification criteria for downhill folders 8 2.3 Lambda repressor as a model system for studying downhill folding 9 2.3.1 Wild-type lambda repressor fragment λ{6-85} 10 2.3.2 Acceleration of λ{6-85} folding by specifific point mutations 11 2.3.3 The incipient-downhill λYA and downhill λHA variants 14 2.4 Single-molecule techniques as a promising tool for probing downhill folding dynamics 17 3 Single-molecule protein folding with optical tweezers 19 3.1 Optical tweezers 19 3.1.1 Working principle of optical tweezers 19 3.1.2 The optical tweezers setup 21 3.2 The dumbbell assay 22 3.3 Measurement protocols 23 3.3.1 Constant-velocity experiments 23 3.3.2 Constant-trap-distance experiments (equilibrium experiments) 24 4 Theory and analysis of single-molecule trajectories 27 4.1 Polymer elasticity models 27 4.2 Equilibrium free energies of protein folding in optical tweezers 28 4.3 Signal-pair correlation analysis 29 4.4 Force dependence of transition rate constants 29 4.4.1 Zero-load extrapolation of rates: the Berkemeier-Schlierf model 30 4.4.2 Detailed balance for unfolding and refolding data 31 4.5 Direct measurement of the energy landscape via deconvolution 32 II Results 33 5 Efficient strategy for protein-DNA hybrid formation 35 5.1 Currently available strategies for protein-DNA hybrid formation 35 5.2 Novel assembly of protein-DNA hybrids based on copper-free click chemistry 37 5.3 Click-chemistry based assembly preserves the native protein structure 40 5.4 Summary 42 6 Non-equilibrium mechanical unfolding and refolding of lambda repressor variants 45 6.1 Non-equilibrium unfolding and refolding of lambda repressor λWT 45 6.2 Non-equilibrium unfolding and refolding of incipient-downhill λYA and downhill λHA variants of lambda repressor 48 6.3 Summary 52 7 Equilibrium unfolding and refolding of lambda repressor variants 53 7.1 Importance of the trap stiffness to resolve low-force nanometer transitions 54 7.2 Signal pair-correlation analysis to achieve millisecond transitions 56 7.3 Force-dependent equilibrium kinetics of λWT 59 7.4 Equilibrium folding of incipient-downhill λYA and downhill λHA variants of lambda repressor 61 7.5 Summary 65 8 Model-free energy landscape reconstruction for λWT, incipient-downhill λYA and downhill λHA variants 69 8.1 Direct observation of the effect of a single mutation on the conformational heterogeneity and protein stability 71 8.2 Artifacts of barrier-height determination during deconvolution 75 8.3 Summary 76 9 Conclusions and Outlook 79