Les objectifs de cette thèse visent le développement d’un traitement inédit dans un repère spatiale tridimensionnel, pour le problème de la dynamique de collisions diffusives d’objets macromoléculaires en solution en écoulement hydrodynamique à l'intérieur des pores de largeur variable, soumis aux forces hydrodynamiques, du mouvement brownien et des collisions diffusifs aux parois des pores, en utilisant la modélisation théorique et les simulations numériques. L’approche par simulation numérique est nécessaire car il est extrêmement complexe d’utiliser des outils analytiques à présent pour traiter le problème de ces collisions diffusives aux parois solides. Les algorithmes que nous avons développés et les simulations correspondantes sont suffisamment généraux et avancés pour être directement appliquée à l'étude de la dynamique d'une grande variété de polymère et des particules biologiques dans des solutions diluées sous diverses conditions physiques et hydrodynamiques à l'intérieur des pores. Par ailleurs, les mécanismes conduisant à l'adhésion de nano particules et de particules macromoléculaires sous conditions de non-équilibre, en raison de l'influence contradictoire des collisions mécaniques diffusifs et les forces attractives de Hamaker aux parois solides, sont d'un intérêt majeur. Nous avons donc développé un modèle théorique pour calculer le coefficient de restitution. L'objectif est de quantifier le bilan énergétique pendant le processus de collision diffusive de ces particules aux parois, sous l'influence des forces de répulsion d'une part et les forces attractives de Hamaker. Cela se fait par l'élaboration d'un modèle, basé sur le JKR et les théories d’Hertz, pour tenir compte des pertes d'énergie lors des collisions et des gains d'énergie en raison des interactions Hamaker. L’adhésion arrive si le bilan énergétique le permet. Notre modèle théorique est développé en proposant une approche particulière basée sur le potentiel Hamaker. Nous démontrons ce bilan par le biais d'une équation caractéristique non linéaire pour le coefficient de restitution, et analysons ses propriétés qui déterminent l'adhésion ou non pour diverses conditions physiques initiales. / The purpose of this thesis is to develop a comprehensive model analysis in a three-dimensional spatial frame for the dynamics of molecular particles in dilute colloidal suspensions in solutions flowing inside pores of variable width, subject to hydrodynamic forces, Brownian motion and diffusive collisions at the rough pore boundaries, by using numerical simulations. The approach by simulations is necessary because it is extremely complex to use analytical tools at present to deal with the problem of diffusive collisions of the particles at the solid pore boundaries. The algorithms which we have developed and the corresponding simulations are sufficiently general and refined to be directly applied to the study of the dynamics of a wide variety of polymer and biological particles in dilute solutions under diverse physical and applicable hydrodynamic conditions inside pores. Moreover, the mechanisms leading to the adhesion of particles of nano sizes under what would be non-equilibrium conditions, due to the conflicting influence of the mechanical diffusive collisions and the attractive Hamaker forces at the boundaries, are of major interest. We have hence investigated a theoretical model to calculate the restitution coefficient from basic physical principles. The objective is to quantify the energy balance during the process of a diffusive collision of a nano particle under the influence of the repulsive forces on one hand, and the attractive Hamaker forces acting on the nano particle on the other. This is done by developing a model, based on the JKR and Hertz theories, to account for the energy losses during collisions, and for the energy gains due to the Hamaker interactions. Adhesion becomes an outcome if the energy balance permits this. Our theoretical model is developed by proposing a special analytic approach based on the Hamaker potential. We derive from the theoretical analysis a characteristic nonlinear equation for the restitution coefficient, and analyze its properties which determine under given physical conditions the outcome for adhesion or not.

Ce travail de thèse s’inscrit dans le cadre du projet ISS/FSL/FASES dont l’objectif est de comprendre les mécanismes de vieillissement des émulsions en microgravité. Ce manuscrit est dédié à l’étude au sol des émulsions de ce projet et notamment de celles stabilisées par des mélanges tensioactifs/nanoparticules. Ces émulsions sont diluées et constituées d’une phase continue d’huile de paraffine et d’une phase dispersée aqueuse contenant un tensioactif et des nanoparticules. Leur étude et leur caractérisation est réalisée par microscopie tomographique optique et cryo-microscopie électronique à balayage. Une étude préalable de la phase dispersée permet de démontrer que les proportions respectives en tensioactif et nanoparticules modifient les propriétés rhéologiques et microscopiques de ces mélanges. Ces modifications permettent de caractériser le couplage entre les molécules tensioactives et les nanoparticules. Lorsque cette phase dispersée est émulsifiée dans l’huile de paraffine, une transition dans la morphologie des gouttes peut être mise en évidence. Les gouttes de phase dispersée présentent une topologie dépendante du ratio des concentrations en tensioactif et nanoparticules : de sphérique (pour les grandes valeurs de ce ratio) elles deviennent polymorphes (pour les petites valeurs). L’observation de ces émulsions en cryo-microscopie électronique à balayage permet de visualiser des microstructures de nanoparticules et d’expliquer l’origine de la déformation des gouttes. / This thesis is part of the ISS/FSL/FASES project which aims at understanding emulsion ageing mechanisms in microgravity. This manuscript is dedicated to the ground study of these emulsions, and particularly to those stabilized by surfactant/nanoparticles mixtures. These emulsions are diluted and composed of a paraffin oil continuous phase and an aqueous dispersed phase composed of the surfactant/particle mixtures. Emulsion characterization is performed with optical tomographic microscopy and cryo-scanning electron microscopy. A preliminary investigation of the dispersed phase shows that the proportion of surfactant and nanoparticles changes the rheological and microscopic properties of these mixtures. These changes allow the characterization of the coupling between surfactant molecules and nanoparticles. When these mixtures are emulsified in paraffin oil, a transition in the droplets morphology is evidenced. Indeed, dispersed phase droplets exhibit different shapes depending on the ratio of surfactant and nanoparticle concentrations: from spherical (for high ratios) they become polymorphous (for small ratios). Observations of these emulsions with cryo-scanning electron microscopy show the existence of nanoparticles microstructures that helps the understanding of the origin of droplets deformation.

Les objectifs de cette thèse visent le développement d'un traitement inédit dans un repère spatiale tridimensionnel, pour le problème de la dynamique de collisions diffusives d'objets macromoléculaires en solution en écoulement hydrodynamique à l'intérieur des pores de largeur variable, soumis aux forces hydrodynamiques, du mouvement brownien et des collisions diffusifs aux parois des pores, en utilisant la modélisation théorique et les simulations numériques. L'approche par simulation numérique est nécessaire car il est extrêmement complexe d'utiliser des outils analytiques à présent pour traiter le problème de ces collisions diffusives aux parois solides. Les algorithmes que nous avons développés et les simulations correspondantes sont suffisamment généraux et avancés pour être directement appliquée à l'étude de la dynamique d'une grande variété de polymère et des particules biologiques dans des solutions diluées sous diverses conditions physiques et hydrodynamiques à l'intérieur des pores. Par ailleurs, les mécanismes conduisant à l'adhésion de nano particules et de particules macromoléculaires sous conditions de non-équilibre, en raison de l'influence contradictoire des collisions mécaniques diffusifs et les forces attractives de Hamaker aux parois solides, sont d'un intérêt majeur. Nous avons donc développé un modèle théorique pour calculer le coefficient de restitution. L'objectif est de quantifier le bilan énergétique pendant le processus de collision diffusive de ces particules aux parois, sous l'influence des forces de répulsion d'une part et les forces attractives de Hamaker. Cela se fait par l'élaboration d'un modèle, basé sur le JKR et les théories d'Hertz, pour tenir compte des pertes d'énergie lors des collisions et des gains d'énergie en raison des interactions Hamaker. L'adhésion arrive si le bilan énergétique le permet. Notre modèle théorique est développé en proposant une approche particulière basée sur le potentiel Hamaker. Nous démontrons ce bilan par le biais d'une équation caractéristique non linéaire pour le coefficient de restitution, et analysons ses propriétés qui déterminent l'adhésion ou non pour diverses conditions physiques initiales.

L'utilisation de chrome hexavalent comme inhibiteur de corrosion dans les revêtements protecteurs de pièces métalliques sera bientôt interdit car cet élément est considéré comme cancérigène et mutagène. L'une des stratégies proposées pour remédier à ce problème est l'incorporation de nano-réservoirs contenant des inhibiteurs de corrosion, autres que le chrome, dans une matrice de revêtement. L'approche utilisée dans ce travail est basée sur la physisorption de l'inhibiteur de corrosion sur des nano-particules chargées. C'est une approche électrochimique où un sel, l'inhibiteur de corrosion, est adsorbé sur la surface des nano-particules chargées. Après l'incorporation de nano-réservoirs chargés dans la matrice de revêtement et le dépôt du film sur le substrat, la morphologie finale, et donc l'homogénéité, du film dépend de plusieurs paramètres tels que la vitesse d'évaporation du film et les interactions entre particules. Par conséquent, il faut s'assurer que les nano-réservoirs sont dispersés de manière homogène à l'intérieur du revêtement ou être en mesure de prédire où les inhomogénéités vont se développer. Ainsi, le premier objectif de ce travail est de développer une stratégie de modélisation pour étudier l'écoulement de suspensions contenant des nano-particules dans des solutions électrolytiques. Les interactions prises en compte ici sont d'origine hydrodynamique, thermique et électrostatique. Nous montrons que dans le cas du séchage d'un film contenant des nano-particules, les interactions pertinentes sont celles d'origine thermique et électrostatique seulement. Sur la base de ce résultat, l'exemple d'un micro-évaporateur est présenté dans lequel des expériences numériques du séchage d'une suspension de nano-particules avec différentes charges de surface ont été réalisées. Sachant que les interactions entre particules sont influencées surtout par la charge et la concentration de l'électrolyte dans la suspension, il existe une réelle motivation pour étudier ces interactions dans les systèmes de nano-particules synthétisées en vue de la conception de nano-réservoirs. Par conséquent, le deuxième objectif de ce travail est de synthétiser des nano-réservoirs de boehmite, d'étudier leur stabilité dans une gamme de concentration d'inhibiteur de corrosion, et finalement de valider ce type de nano-réservoirs pour des applications de revêtements anti-corrosion. / The use of hexavalent Chromium as a corrosion inhibitor in protective coat-ings of metal parts will soon be prohibited because this element is consideredcarcinogenic and mutagenic. One of the strategies suggested to overcomethis problem is the incorporation of nano-containers containing corrosion in-hibitors, other than Chromium, inside a coating matrix. The nano-containersapproach used in this work is based on the physisorption of the corrosioninhibitor on charged nano-particles. It is an electrochemical approach wherea salt, the corrosion inhibitor, is adsorbed on the surface of the charged nano-particles. After the incorporation of the charged nano-containers in the coat-ing matrix and the deposition of the film on the substrate, the final morphol-ogy and therefore the homogeneity of the film will depend on several pa-rameters such as the evaporation rate and the interactions between particles.Consequently, one has to insure that the nano-containers are homogeneouslydispersed inside the coating matrix after the deposition, or be able to predictwhere inhomogeneities will develop. Hence, the first aim of this work is todevelop a modeling strategy to study the flow of suspensions containing in-teracting nano-particles in electrolyte solutions. The interactions taken intoaccount here are of hydrodynamic, thermal, and electrostatic origin and itis argued that in the application of film drying of nano-particles the interac-tions relevant are those of thermal and electrostatic origin only. Based onthis idea, the simulation of the drying of a suspension with nano-particles ofdifferent charges has been realized in a micro-evaporator. Considering thatparticle interactions are influenced by the charge and the electrolyte con-centration of the suspension, there is a clear motivation to study these in-teractions in a synthesized system of nano-particles, candidate in the designof nano-containers. Therefore, the second aim of this work is to synthe-size boehmite nano-containers, study their stability in a range of corrosioninhibitor concentration, and finally qualify them as candidates for the appli-cation of anti-corrosion coatings.

Les catalyseurs bifonctionnels pour l’hydrocraquage nécessitent à la fois des sites acides de Brønsted et des sites métalliques. L’intimité entre sites acides et sites métalliques peut donc influer sur l’activité et la sélectivité de la réaction. Nous nous sommes proposés d’explorer l’effet de la distance sites métalliques-sites acides sur la conversion du n-heptane en concevant des catalyseurs à base de platine supportés sur des nanostructures alumine-zéolithe. Pour cela, nous avons étudié la synthèse de suspensions colloïdales nanométriques de zéolithes NaY (20 nm) beta (30 nm), ZSM-5 (50 nm). Des matériaux composites ont ensuite été préparés, soit par synthèse directe en présence d’un support, soit par mise en contact de ces suspensions colloïdales (dans les conditions appropriés de pH) avec des suspensions de boehmite (se transformant en γ-alumina par calcination). Des composites cœur-zéolithe@couronne(alumine) ont ainsi été obtenus. Les particules de platine ont été par la suite sélectivement formées sur les domaines alumine ou zéolithe de ces composites en utilisant le précurseur approprié de platine dans un domaine de pH adapté (pH=5-8). Les catalyseurs ainsi préparés ont été comparés à d’autres catalyseurs pour lesquels la distance entre sites acides et sites métalliques varie entre le nm et le μm, pour former une série de catalyseurs avec des distances métal-acide et des accessibilités aux sites différentes. L’étude catalytique a permis de conclure que l’amélioration de l’accessibilité aux sites actifs (Pt0/Alumine-nanozéolithe) améliore la sélectivité a vers les produits d’isomérisation, alors que la distance ne joue un rôle inhibiteur que quand elle atteint une échelle de plusieurs μm. / Bifunctional hydrocracking catalysts require both Brønsted acid sites and metal sites. Hence, the intimacy between acid sites and metal sites can influence the activity and selectivity of the reaction. We intended to explore the effect of metal sites-acid sites distance on the conversion of n-heptane by designing platinum catalysts supported on alumina-zeolite nanostructures. For this, we studied the synthesis of nanoscale colloidal suspensions of zeolite NaY (20 nm) beta (30 nm), ZSM-5 (50 nm). Composite materials were then prepared either by direct synthesis in the presence of a support, or by contacting these colloidal suspensions (at appropriate pH conditions) with suspensions of boehmite (turning into γ-alumina by calcination). Zeolite-core@alumina-crown composite crown) were thus obtained. The platinum particles were thereafter selectively formed on the alumina or zeolite domains of these composites using the appropriate precursor of platinum in a suitable pH range (pH = 5-8). The thus-prepared catalysts were compared with other catalysts, for which the distance between the acid sites and the metal sites varies between nm and μm scales, to form a series of catalysts with variable acid-metal distances and accessibilities. Catalytic study concluded that improving accessibility to the active sites (Pt0 / Alumina-nanozéolithe) improves the selectivity to isomerization, while the distance plays an inhibitory role only when it reaches a scale of several microns.

Ce travail de thèse de doctorat propose et évalue différentes solutions pour caractériser, avec des outils optiques et électromagnétiques non intrusifs, les nanoparticules et agrégats observés dans différents systèmes physiques : suspensions colloïdales, aérosols et plasma poussiéreux. Deux types de modèles sont utilisés pour décrire la morphologie d'agrégats fractals (p. ex. : suies issues de la combustion) et agrégats compacts (qualifiés de « Buckyballs » et observés dans des aérosols produits par séchage de nano suspensions). Nous utilisons différentes théories et modèles électromagnétiques (T-Matrice et approximations du type dipôles discrets) pour calculer les diagrammes de diffusion (ou facteur de structure optique) de ces agrégats, de même que leurs spectres d'extinction sur une large gamme spectrale. Ceci, dans le but d'inverser différentes données expérimentales. Différents outils numériques originaux ont également été mis au point pour parvenir à une analyse morphologique quantitative de clichés obtenus par microscopie électronique. La validation expérimentale des outils théoriques et numériques développés au cours de ce travail est focalisée sur la spectrométrie d'extinction appliquée à des nano agrégats de silice, tungstène et silicium. / This Ph.D. work provides and evaluates various solutions to characterize, with optical/electromagnetic methods nanoparticles and aggregates of nanoparticles found in suspensions, aerosols and dusty plasmas. Two main models are introduced to describe the morphology of particle aggregates with fractal-like (for particles in plasmas and combustion systems) and Buckyballs-like (aerosols, suspensions) shapes. In addition, the author proposes various solutions and methods (T-Matrix, Rayleigh type approximations) to calculate the scattering diagrams (optical structure factors) of fractal aggregates as well as algorithms to inverse extinction spectra. As a reference case for the performed analysis, several tools to describe the morphology of fractal aggregates from electron microscopy images have been also developed. The experimental validation carried out with the Light Extinction Spectrometry (LES) technique (for nano silica beads, tungsten, dusty plasma and silicon aggregates) clearly proves the validity of the algorithms developed as well as the potential of the LES technique.

‘Soft condensed matter’ is a newly-emerged sub-discipline of physics concerned with the study of systems that are mechanically soft such as colloids, emulsions, surfactants, polymers, liquid crystals, granular media and various biomaterials including DNA and proteins. These materials display a broad range of interesting microstructures and phase behaviours and have a myriad of applications in the materials, food, paint and cosmetic industries as well as medical technologies. Soft condensed matter physics presents new opportunities and challenges for the development of new ideas and concepts in experimental and theoretical physics alike. Because the field overlaps with many different disciplines, the study of soft matter also offers promising developments to other fields of science including chemistry, chemical engineering, materials science, biology, and environmental science. The behaviour of these systems is dominated by one simple fact: they contain mesoscopic structures in the size range 10 nm to 1 µm that are held together by weak entropic forces. The elastic constants of these materials are 109 times smaller than the conventional atomic materials and hence are easily deformable by external stresses, electric or magnetic fields, or even by thermal fluctuations. We have studied two important classes of soft matter systems in this thesis -colloidal suspensions and surfactant systems. The thesis is divided into two main themes: (a) Effects of electric field on the colloidal suspensions, and (b) Effects of shear on surfactant solutions. Motions of colloidal particles under the influence of applied electric field were observed under a microscope and were studied using image analysis and particle tracking. We have also used tracking of thermal fluctuations of colloidal particles embedded in surfactant gels to study microrheology of surfactant solutions. Linear and non-linear rheology of aqueous solutions of cationic cetyltrimethyl ammonium bromide (CTAB) and anionic sodium-3-hydroxynapthalene-2-carboxylate (SHNC) were studied using bulk rheology in a commercial rheometer. Rheological studies of an anionic surfactant sodium dodecyl sulphate (SDS) in the presence of strongly binding counterion p-toluidine hydrochloride (PTHC) has also been done. Chapter 1 starts with a general introduction to soft condensed matter systems and then we proceed to describe two specific class of soft condensed materials which we have studied in this thesis -colloidal suspensions and surfactant/water systems. After describing different types of colloids, we discuss why colloids are suitable as model systems in condensed matter physics. This is followed by a discussion on the chemical structure, phase behaviour and self assembling properties of surfactant molecules in water. We then discuss the inter-macromolecular forces such as van der Waals interaction, the screened Coulomb repulsion, hydrogen bond, hydrophobic and hydration forces and steric repulsion which are the major players in the interaction in soft condensed matter systems. The systems that have been the subject of our experimental studies, viz. polystyrene colloidal suspensions, CTAB+SHNC, SDS+PTHC and CTAT have also been discussed in detail. Then we have given an overview of effects of electric field on the colloidal suspensions. Two types of geometries have been discussed: one in which the field is parallel to the plates and another when the field is perpendicular to the electrodes. Application of colloidal particles in diagnostic tests (Latex Agglutination Tests) has been discussed after this. Some methods used to enhance the sensitivity of LATs have also been reviewed. This is followed by a theoretical background of linear and non-linear rheology. We have also given an introduction to digital video microscopy, its advantages and discussed few quantities like pair correlation function, structure factor which can be extracted using digital video microscopy and particle tracking. The concluding part of this chapter describes the organization of this thesis. Chapter 2 discusses the experimental apparatus and techniques used in our studies. We describe our setup for applying the electric field to the colloidal particles and imaging and tracking their motion. We also discuss the image processing and analyzing methods for extracting the useful quantities from the digitized images. We have described the various components of the MCR-300 stress-controlled rheometer (Paar Physica, Germany) and the AR-1000N stress-controlled rheometer (T. A. Instruments, U. K.) followed by different experimental geometries that we have used for our experiments. Next we have described the various experiments that can be done using a commercial rheometer. Calculation of surface charge of colloidal particles using a conductivity meter has been demonstrated for our colloidal particle suspensions. We also describe the sample preparation methods employed in different experiments. In Chapter 3, we have discussed our study of clustering of colloidal particles under the influence of an ac electric field as a function of frequency. The field was applied in a direction perpendicular to the confining walls. Two regimes are observed, a low frequency regime where the clusters are isotropic with a local triangular order and a new high-frequency regime where the clusters are highly elongated (anisotropic) with no local order. The crossover from one regime to the other occurs at a critical frequency, fc. The formation of elongated clusters seen at high frequencies is explained in terms of rotation of particles due to a phase lag between the polarization of the electric double layer around a particle and the applied electric field that arises because of inhomogeneities of the conducting surface. We have also observed that the threshold field for the cluster formation, Eth, increases with frequency in both the regimes. We did these studies on two different sizes of particles and found that both Eth and fc were lower for the larger particles. Our model based on particle rotation was able to estimate the value of fc correctly for both the sizes of the particles. Chapter 4 describes a method employing an ac electric field applied perpendicular to the confining walls to increase the sensitivity of recognition of ligands by their corresponding receptors grafted on Brownian latex particles. Application of electric field assists the colloidal micro-particles grafted with receptors to come nearer due to electro-hydrodynamic drag. This increase in the local concentration of the latex particles results in improving the chances of ligand-receptor interaction leading to the aggregation of the latex particles. With this technique we have been able to increase the sensitivity of the ligand-receptor recognition by a factor as large as 50. We have demonstrated the utility of our method using streptavidin as the model receptor and biotinylated RNase A as the model ligand. We have also applied our technique to a commercially available kit for rheumatoid factor (RF) with successful results. The same method was also successfully applied for the detection of typhoid whose antibodies were purified and attached to polystyrene particles by our collaborators from DRDE Gwalior. In Chapter 5, we have studied the statics and dynamics of colloidal particles at different applied electric fields from zero to beyond the threshold field. We have taken a series of time-lapsed images and calculated out the pair-correlation function, mean squared displacement, structure factor, non-Gaussian parameter etc. We have studied both mono-dispersed colloidal system and binary colloidal system (mixture of two different sizes of particles). The aggregates formed in the two cases were analysed with the help of Voronoi polygons to quantify the microscopic structure. In mono-dispersed system, the aggregates formed were two-dimensional hexagonal crystals and we have used this system to study the freezing transition in 2-dimension. The properties of the system in the liquid and the crystalline state satisfy various criteria for the 2-d freezing transition. The first maximum of the structure factor at the voltage at which freezing occurs, is 5.5 as has been suggested for the 2-d freezing. This is reflected in the dynamics of the system also, where the ratio D/D0 falls below 10%, in accordance with the LPS (L¨owen, Palberg, Simon) criterion for freezing in 2-d colloidal systems [Phys. Rev. Lett. 70, 1557 (1993)]. However, in the binary colloidal system the clusters formed were not crystalline but more like 2-d dense liquids. A closer inspection of these clusters reveals that the motion of a smaller subset of particles is cooperative and follows string-like paths. The mean square displacement of such a system shows a plateau in the intermediate times which indicates the “caging” of particles by its neighbours. A peak in non-gaussian parameter indicates the presence of dynamical heterogeneities in the system. In Chapter 6, we have described the use of multiple particle tracking to study the microrheology of semidilute solutions of wormlike micelles and compared the results with those from macrorheology experiments done on the same samples. Two concentrations of CTAT (1.3% and 2%) were used. We observed that, in spite of the mesh size being much smaller than the size of the probe particles, the viscoelastic response function calculated using the one-point microrheology does not match with that measured from macrorheology. This can be attributed to the fact that there is another important length scale in the system, the mean micellar length, and it is comparable to the probe particle size. Two-point microrheology was successful in verifying the macrorheology results for CTAT 1.3% but it fails to do so for CTAT 2%. We attribute this to the fact that in a higher viscosity sample (2%), the hydrodynamic force propagate to a lesser distance, thereby limiting the measurable correlation between the particles and precluding the success of two-point microrheology. Chapter 7 describes a rheological study of aqueous solutions of varying concentration of cationic cetyltrimethyl ammonium bromide (CTAB) and anionic sodium-3-hydroxynapthalene-2-carboxylate (SHNC) kept at a fixed molar concentration ratio [CTAB]/[SHNC] = 2. At this molar ratio, the surfactants self-assemble into wormlike micelles which get entangled above the overlap concentration to form viscoelastic gel. The range of the total surfactant concentration φ varies from 1.17% to 5.16% by weight. We found that, plateau modulus, G0, shows a power law dependence on the surfactant concentration, φ, with an exponent 3, which is higher than the expected value of 2.25 observed for the one-component wormlike micelles. Zero shear viscosity, η0, and relaxation time, τR show a maximum at the surfactant concentration, φmax = 1.9% in contrast to a monotonic increase with φ. We propose that this non-monotonic behaviour is due to the unusual dependence of the average micellar length L ¯on φ, showing a maximum in average micellar length L at φmax. This argument provides a strong support to the model of micellar growth in the presence of electrostatic interactions developed by Mackintosh et. al [Europhys. Lett. 12, 697 (1990)]. The presence of electrostatic interactions also appears in the behaviour of the plateau modulus G0 that exhibits a larger φ dependence than in highly screened micelles. In the non-linear flow experiments, a minimum observed in critical shear rate (the shear rate at which shear thinning starts), ˙γc, at φmax strengthens our arguments. In Chapter 8, we describe the phase behaviour and rheology of SDS+PTHC (sodium dodecyl sulphate + p-toluidine hydrochloride) micellar solutions at different molar ratios α=[PTHC]/[SDS]) of the two components. At low values of α, polarizing microscopy observations reveal a transition from an isotropic to a nematic phase of disk-like micelles, whereas a transition to a lamellar phase occurs at higher α values > 0.5, on increasing the surfactant content. Linear rheology of the isotropic micellar solution reveal a viscous behaviour over a large range of surfactant concentrations. Surprisingly, this also extends to the nematic phase of disk-like micelles observed at α =0.2 and φ =0.35. These systems also exhibit a viscoelastic behaviour over a narrow range of surfactant concentration as reported in earlier studies. The extent of the viscoelastic region of the isotropic micellar solution also decreases with increase in α. Frequency sweep curves in this region, scaled on to a master curve is reminiscent of dilute suspensions of hard spheres or rigid Brownian rods. Consistent with the results from oscillatory shear measurements, the f;ow behaviour examined under steady shear is Newtonian over a large range of surfactant content in the isotropic micellar solution. An interesting result in these studies is the non-monotonic behaviour of the viscosity with increase in surfactant concentration. It is likely that the sharp rise in viscosity arises from a jamming effect of the rigid rods. Dynamic light scattering studies suggest that the drop in viscosity is due to the decrease in the length of the micellar aggregates. This is followed by a change in the morphology of the micelles from rods to disks as indicated by the transition to a nematic phase of disk-like micelles or a lamellar phase. A change in the morphology of micellar aggregates with increase in α is expected in mixed surfactant systems with strongly binding counterions. However, the surprising result is the change in morphology of the micellar aggregates with surfactant content. Such a behaviour is seen in mixed surfactant systems for the first time. The thesis concludes with a summary of our main results and a brief discussion of the scope of future work in Chapter 9.

Gegenstand dieser Arbeit war das Stabilitätsverhalten von binären kolloidalen Suspensionen mit hohen Feststoffkonzentrationen (z. B. keramische Suspensionen). Dabei wurde die Stabilität mit Hilfe des Sedimentationsverhaltens bewertet und mit dem Grenzflächenzustand korreliert, der als effektives Zetapotenzial erfasst wurde. Die Untersuchungen erfolgten an drei Oxiden mit unterschiedlichen physiko-chemischen Eigenschaften, wobei die Suspensionszusammensetzung und der pH-Wert über weite Bereiche variiert wurden. Ein wesentliches Ergebnis dieser Arbeit besteht im Nachweis, dass die Löslichkeit der einzelnen partikulären Komponenten in den binären Suspensionen zu einer gegenseitigen Beeinflussung der Grenzflächeneigenschaften führt und dadurch das Stabilitätsverhalten des gesamten Systems maßgeblich bestimmt. Von Relevanz ist zudem das Mischungsverhältnis, von dem zum einen das Löse- und Adsorptionsverhalten und zum anderen die Morphologie von Heteroaggregaten abhängt und das auf diese Weise auch für das makroskopische Verhalten entscheidend ist. Die Arbeit zeigt deutlich, dass das Reich der Kolloide neben universellen Mechanismen von stoffspezifischen Phänomenen beherrscht wird. Daraus folgt, dass eine allumfassende Behandlung der Stabilität nicht möglich ist. Vielmehr kann nur an Beispielen demonstriert werden, welche Art von Phänomenen auftreten und wie sie genutzt oder vermieden werden können.

The work presented in this doctoral thesis employs colloidal suspensions to explore key open problems in condensed matter physics. Colloidal suspensions, along with gels, polymers, emulsions and liquid crystals belong to a family of materials that are collectively labelled as soft matter. Compositionally, colloidal suspensions consist of particles whose size ranges from a few nanometers to a few microns, dispersed in a solvent. A hallmark feature of these systems is that they exhibit Brownian motion, which makes them suitable for investigating statistical mechanical phenomena. Over the last fifteen years or so, colloids have been used extensively as model systems to shed light on a wide array of such phenomena typically observed in atomic systems. The chief reason why colloids are good mimics of atomic systems is their large size and slow dynamics. Unlike atomic systems, the dynamics of colloids can be probed in real time with single-particle resolution, which allows one to establish the link between macroscopic behavior and the microscopic processes that give rise to it. Yet another important feature is that colloidal systems exhibit various phases of matter such as crystals, liquids and glasses, which makes them versatile model systems that can probe a broad class of condensed matter physics problems. The work described in this thesis takes advantage of these lucrative features of colloidal suspensions to gain deeper insights into the physics of glass formation as well as shear-induced anisotropic grain growth in polycrystalline materials. The thesis is organized into two preliminary chapters, four work chapters and a concluding chapter, as follows. Chapter 1 provides an introduction to colloidal suspensions and reviews the chief theo-retical concepts regarding glass formation and grain boundary dynamics that form an integral part of subsequent chapters. Chapter 2 describes the experimental methods used for performing the work presented in the thesis and consists of two parts. The first part describes the protocols followed for synthesizing the size-tunable poly (N-isoprolypacrylamide) (PNIPAm) particles used in our study of shear-induced grain growth. The second part describes the instrumentation and techniques, such as holographic optical tweezers, confocal microscopy, rheology and Bragg diffraction microscopy, used to perform the measurements described in the thesis. Chapter 3 deals with our work on the dynamical facilitation (DF) theory of glass forma-tion. Despite decades of research, it remains to be established whether the transformation of a liquid into a glass is fundamentally thermodynamic or dynamic in origin. While obser-vations of growing length scales are consistent with thermodynamic perspectives, the purely dynamic approach of the DF theory has thus far lacked experimental support. Further, for glass transitions induced by randomly freezing a subset of particles in the liquid phase, theory and simulations support the existence of an underlying thermodynamic phase transi-tion, whereas the DF theory remains unexplored. In Chapter 3, using video microscopy and holographic optical tweezers, we show that dynamical facilitation in a colloidal glass-forming liquid grows with density as well as the fraction of pinned particles. In addition, we observe that heterogeneous dynamics in the form of string-like cooperative motion, which is consid-ered to be consistent with thermodynamic theories, can also emerge naturally within the framework of facilitation. These findings suggest that a deeper understanding of the glass transition necessitates an amalgamation of existing theoretical approaches. In Chapter 4, we further explore the question of whether glass formation is an intrinsi-cally thermodynamic or dynamic phenomenon. A major obstacle in answering this question lies in determining whether relaxation close to the glass transition is dominated by activated hopping, as espoused by various thermodynamic theories, or by the correlated motion of localized excitations, as proposed in the Dynamical Facilitation (DF) approach. In Chapter 4, we surmount this central challenge by developing a scheme based on real space micro-scopic analysis of particle dynamics and applying it to ascertain the relative importance of hopping and facilitation in a colloidal glass-former. By analysing the spatial organization of excitations within cooperatively rearranging regions (CRRs) and examining their parti-tioning into shell-like and core-like regions, we establish the existence of a crossover from a facilitation-dominated regime at low area fractions to a hopping-dominated one close to the glass transition. Remarkably, this crossover coincides with the change in morphology of CRRs predicted by the Random First-Order Transition theory (RFOT), a prominent ther-modynamic framework. Further, we analyse the variation of the concentration of excitations with distance from an amorphous wall and find that the evolution of these concentration profiles with area fraction is consistent with the presence of a crossover in the relaxation mechanism. By identifying regimes dominated by distinct dynamical processes, our study offers microscopic insights into the nature of structural relaxation close to the glass transi-tion. In Chapter 5, we extend our investigation of the glass transition to systems composed of anisotropic particles. The primary motivation for this is to bridge a long-standing di-vide between theories and simulations on one hand, and experiments on molecular liquids on the other. In particular, theories and simulations predominantly focus on simple glass-formers composed of spherical particles interacting via isotropic interactions. Indeed, even the prominent theory of Dynamical Facilitation has not even been formulated to account for anisotropic shapes or interactions. On the other hand, an overwhelming majority of liquids possess considerable anisotropy, both in particle shape as well as interactions. In Chapter 5, we mitigate this situation by developing the DF theory further and applying it to systems with orientational degrees of freedom as well as anisotropic attractive interactions. By analyzing data from experiments on colloidal ellipsoids, we show that facilitation plays a pivotal role in translational as well as orientational relaxation. Further, we demonstrate that the introduction of attractive interactions leads to spatial decoupling of translational and rotational facilitation, which subsequently results in the decoupling of dynamical het-erogeneities. Most strikingly, the DF theory can predict the existence of reentrant glass transitions based on the statistics of localized dynamical events, called excitations, whose duration is substantially smaller than the structural relaxation time. Our findings pave the way for systematically testing the DF approach in complex glass-formers and also establish the significance of facilitation in governing structural relaxation in supercooled liquids. In Chapter 6, we turn our attention away from the glass transition and address the problem of grain growth in sheared polycrystalline materials. The fabrication of functional materials via grain growth engineering implicitly relies on altering the mobilities of grain boundaries (GBs) by applying external fields. While computer simulations have alluded to kinetic roughening as a potential mechanism for modifying GB mobilities, its implications for grain growth have remained largely unexplored owing to difficulties in bridging the disparate length and time scales involved. In Chapter 6, by imaging GB particle dynamics as well as grain network evolution under shear, we present direct evidence for kinetic roughening of GBs and unravel its connection to grain growth in driven colloidal polycrystals. The capillary fluctuation method allows us to quantitatively extract shear-dependent effective mobilities. Remarkably, our experiments reveal that for sufficiently large strains, GBs with normals parallel to shear undergo preferential kinetic roughening resulting in anisotropic enhancement of effective mobilities and hence directional grain growth. Single-particle level analysis shows that the anisotropy in mobility emerges from strain-induced directional enhancement of activated particle hops normal to the GB plane. Finally, in Chapter 7, we present our conclusions and discuss possible future directions.

L’indisponibilité d’un transformateur de puissance a de fortes répercussions financières aussi bien pour les exploitants de réseaux d’énergie électriques que pour les clients qui y sont connectés. Afin de prévenir les pannes et d’optimiser la performance de ces équipements d’importance stratégique, de nombreuses techniques et outils de diagnostic ont été développés. L’huile contient environ 70 % des informations de diagnostic sur l’état des transformateurs. Le défi consiste à y accéder et à les utiliser efficacement. L’atteinte d’un tel objectif passe nécessairement par des techniques de diagnostic fiables. En plus des techniques traditionnellement utilisées, trois nouvelles techniques de diagnostic issues des normes ASTM sont utilisées : (1) le test de stabilité qui permet de simuler le comportement sous champ électrique d’une huile en fournissant des informations sur la qualité de celle-ci ; (2) la spectrophotométrie UV/Visible qui permet de mesurer la quantité relative de produits de décomposition dissous dans l’huile ; et (3) la turbidité qui mesure la pureté d’une huile neuve ou usagée. Une méthode quantitative permettant de déterminer les paramètres affectant la formation du soufre corrosif sur les conducteurs en cuivre dans les transformateurs de puissance est proposée. Il est montré entre autres que la tendance au gazage des esters naturels est plus faible que celle de tous les autres types d’huile (minérales, esters synthétiques, silicone). La turbidité et la spectrophotométrie UV/Visible permettent de quantifier efficacement les contaminants qui résultent de l’action d’une décharge électrique sur l’huile isolante. Un nombre important de cycles de régénération (au moins 15) est nécessaire pour qu’une huile vieillie en service retrouve les aptitudes d’une huile neuve. Une nouvelle technique de régénération est présentée pour réduire le nombre de cycles de régénération ; celle-ci consiste à utiliser la terre à foulon traitée avec de l’azote. Il est montré également que le temps constitue le paramètre le plus nuisible dans la formation de soufre corrosif. L’action combinée du temps et de l’agressivité de l’oxygène dissous l’accélère fortement. / A power transformer outage has a dramatic financial consequence not only for electric power systems utilities but also for interconnected customers. In order to prevent any failure and to optimize their maintenance, various diagnostic techniques and tools have been developed. Insulating oil contains about 70% of diagnostic information on the transformer condition. The challenge is to access and use them efficiently. To meet this objective reliable diagnostic techniques are required. In addition to traditional testing methods, three recently developed ASTM testing techniques were used: (1) oil stability testing that simulates the behaviour of oil under electrical stress by providing information on its quality; (2) the UV/Visspectrophotometry that measures the amount of the relative dissolved decay products in insulating oil; and (3) the turbidity that measures the purity of virgin and aged oil. A quantitative laboratory technique capable of determining the parameters affecting the formation of corrosive sulphur deposition on copper conductors in power transformer is proposed. It is shown among other that the gassing tendency of natural esters is lower than that of the other types of insulating fluids (mineral oil, synthetics esters and silicone oil). The turbidity and UV/Vis spectrophotometry allow quantifying effectively, the relative amount of contaminants resulting from electrical discharge in oils. A large number of reclamation cycles (around 15 passes) are required for in-service aged oil to regenerate to the level of new oil. Anew technique enabling reducing the number of reclamation cycles is proposed; this latter consists in the use of Fuller’s Earth previously treated with dry nitrogen. It is also shown that time is the most influential parameter in the formation of corrosive sulfur. The process is accelerated when time and aggressiveness of oxygen are partnered.