Yes / Polypropylene (PP) reinforced with 2 and 4 wt% of multi-walled carbon nanotubes (MWNT) were melt-blended in twin screw extruder and then molded by compression or micromolding process. The impact of injection speed on the surface morphology, rheological and tensile characteristics was investigated by using a scanning electron microscope, parallel plate rheometry, and tensiometry. Results showed that the tensile properties of micro-molded specimens were remarkably higher than those of the compression molded sheets. Compared to compression molded sheets, micromolded specimens demonstrated up to 40 and 244% higher tensile stiffness and yield strength, respectively, most likely due to the alignment of polymer chain segments in the flow direction induced during the micromolding process. It was observed that the fast filling speed caused a drop in the tensile properties of the nanocomposites and polymer. Rheological examination revealed that the presence of a rheological percolation network in the nanocomposites produced by micromolding and the fast injection speed was beneficial for establishing the percolated network. Morphological examination revealed that the size of nanotube agglomerations that appeared in micromolded specimens was up to five times smaller than in compression molded sheets and the agglomeration size decreased with the increase of the injection speed.

Flexible high-deflection strain gauges have been demonstrated as cost-effective and accessible sensors for capturing human biomechanical deformations. However, the interpretation of these sensors is notably more complex compared to conventional strain gauges, partially owing to the viscoelastic nature of the strain gauges. On top of the non-linear viscoelastic behavior, dynamic resistance response is even more difficult to capture due to spikes in resistance during strain changes. This research examines the relationships between stress, strain, and resistance in nanocomposite sensors during dynamic strain situations. Under the assumption that both macroscopic stress and resistance are governed by microscopic stress concentrations at the junctions between nanoparticles and silicone matrix, the stress-resistance relationship is analyzed. Both stress and resistance are found to exhibit aspects of viscoelastic behavior, including creep decay and relaxation during constant strains. However, the resistance spikes are found to be more complex than a simple stress-resistance model can capture. This research then develops a model that captures the strain-resistance relationship of the sensors, including resistance spikes, during cyclical movements. The forward model, which converts strain to resistance, is comprised of four parts to accurately capture the different aspects of the sensor response: a quasi-static linear model, a spike magnitude model, a long-term creep decay model, and a short-term decay model. An inverse problem approach is used to create an inverse model, which predicts the strain vs time data that would result in the observed resistance data. The model is calibrated for a particular sensor from a small amount of cyclic data from a single test. The resulting sensor-specific model is able to accurately predict the resistance output with an R-squared value of 0.90. The inverse model is able to accurately predict key strain characteristics with a percent error of 0.5. The model can be used in a wide range of applications, including biomechanical modeling and analysis. It is found that the resistance spikes are directly correlated to the strain acceleration in terms of timing and in terms of magnitude. Poisson contraction rates and voids in the material are possible causes for resistance spikes during dynamic strain movements.

Le processus de photocatalyse est l'un des moyens prometteurs d'utiliser l'énergie solaire à grande échelle pour différents types d'applications tels que la production d'hydrogène comme énergie propre ou encore la purification de l'eau et l'air contre les polluants et les produits chimiques nocifs. Néanmoins, le pourcentage de l’énergie du rayonnement solaire utilisé est généralement inférieur à 1%, en raison de la faible absorption de la lumière solair, de la rapide recombinaison de charge « électron-trou paires » et de l'instabilité photochimique. La modification de la structure des semi-conducteurs et la création de photocatalyseurs nanocomposites peuvent aider à surmonter ces problèmes. Le TiO2 est le photocatalyseur le plus étudié en raison de ses propriétés physiques et chimiques imortantes dans le processus de photocatalyse. Bien que son faible coût encourage à l'utiliser à grande échelle, sa largeur de bande interdite (EG =3.2 eV) importante, qui ne peut être activée que par irradiation UV, et sa vitesse de recombinaison des charges, ont limité son utilisation dans les applications industrielles. La création d'une hétérojonction entre TiO2 et d'autres semiconducteurs actifs sous la lumière visible est l’un des moyens les plus prometteurs pour utiliser les propriétés du dioxyde de titane dans la région du visible. De plus, le nitrure de carbone graphitique (g-C3N4) a été largement étudié pour la production d'hydrogène sous irradiation lumineuse visible. Malgré le fait qu'il peut être actif dans la région du visible et réduire les protons pour générer de l'hydrogène, son efficacité est considérablement limitée en raison de son taux de recombinaison de charge élevé et de sa faible surface spécifique. Nous avons synthétisé un photocatalyseur nanocomposite de g-C3N4 et TiO2 afin d’améliorer la procédure de séparation des charges et donc de produire plus d'hydrogène. Des nanodisques de titanate uniformes (TND) avec un diamètre compris entre 12 et 35 nm ont été synthétisés à l’aide d’une méthode solvothermale. Les feuilles nanométriques de g-C3N4 ont été synthétisés par des techniques de sonication, puis ont été mélangées avec des TND. Après cela, une étape de calcination a non seulement généré des contacts intimes avec deux semi-conducteurs, mais aussi converti les TND en nanoparticules de TiO2. En raison de la position des bandes de valence et de conduction des deux semi-conducteurs, les électrons photogénérés sont en mesure de passer du g-C3N4 au TiO2. Grâce à l’ajout de Pt comme cocatalyseur ainsi que comme fournisseur de sites actifs, les électrons photoexcités sont en capacité de réduire les protons de l'eau et de générer du dihydrogène. Cette hétérojonction pourrait produire plus du double l’hydrogène que le gC3N4 pur dans les mêmes conditions. Nous avons créé une nouvelle forme de feuille nanométrique de g-C3N4 contenant des lacunes de carbone avec des trous dans tous les plans de feuille. Après la synthèse du matériau de vrac g-C3N4 à partir du dicyandiamide, le matériau obtenu a été chauffé à 650 ° C sous argon pendant 2 h. Après avoir refroidi, il a été calciné à nouveau à 500 ºC pendant 2 heures sous air. Ainsi, sa surface spécifique a été considérablement augmenté de 28 m2.g-1 de g-C3N4 à 160 m2.g-1. En outre, ces traitements par étapes ont introduit certains défauts tels que des lacunes de carbone à l'intérieur de la structure des feuilles nanométriques de g-C3N4. Ces derniers ont fourni des sites photocatalytiques hautement actifs pour l'évolution de l'hydrogène. Par conséquent, sa production d'hydrogène est dix fois supérieure à celle du g-C3N4 brut sous irradiation de la lumière visible. Il a montré une efficacité quantique très élevée de 29,2% et 21,3% à 400 nm et 420 nm, respectivement. Enfin, nous avons généré une solution solide de zinc-cadmium (ZnxCd1-xS) par synthèse solvothermale en utilisant des précurseurs de glycérates métalliques de Cd et Zn. Ensuite, le matériau a été calciné (500 ºC pendant 4 heures) et traité avec H2S à 450 ºC pendant 2 heures. Ainsi, une solution solide homogène de ZnxCd1-xS avec structure cristallographique de wurtzite hexagonale a été formée. Il convient de mentionner que le semi-conducteur obtenu peut absorber une large partie du spectre visible, de plus, sa largeur de bande interdite est fortement affecté par le rapport Zn / Cd et varie entre 2,35 et 3,4 eV (0≤x≤1). Les meilleurs résultats pour l'évolution de l'hydrogène ont été obtenus à partir de l'échantillon Zn30Cd70S avec dépôt de MoS2 comme cocatalyseur. Il peut générer de l'hydrogène dans des longueurs d'onde les plus longues de la région de la lumière visible et ses rendements quantiques sont : 46,6% à 400 nm à 23,4% à 500 nm ainsi que 11,3% à 550 nm. / Photocatalysis process is one of the promising ways to use solar energy in large scale for various kind of application including producing hydrogen as clean energy and purify water and air from harmful pollutants and chemicals. Nevertheless, the solar conversion efficiency of photocatalysts are usually below 1% because of weak sunlight absorption, high charge recombination and high photochemical instability. Modifying semiconductor structure and creating nanocomposite photocatalyst can help to overcome these issues. TiO2 is the most well-known photocatalysts because of its physical and chemical properties in photocatalysis process. Although its low cost encourages people to utilize it in large scale, its large band gap, which can only be activated under UV irradiation, and high rate of charge recombination, limited its usage in industrial applications. Creating an heterojunction between TiO2 and others visible light active semiconductor, is one of the best way to take advantage of TiO2 in visible region. Furthermore, graphitic carbon nitride (g-C3N4) has been widely investigated for its potential in hydrogen production under visible light irradiation. Despite the fact that it can activated in visible light region and reduce protons to generate hydrogen, its efficiency is considerably limited because of its high rate of charge recombination and low specific surface area. We synthesized a nanocomposite photocatalyst of g-C3N4 and TiO2 in order to increase charge separation procedure and so it can produce more hydrogen. Uniform titanate nanodisks (TNDs) with diameter between 12 and 35 nm were synthesized with a solvothermal method. Nanosheets of g-C3N4 were synthesized via sonication techniques and then were mixed with TNDs. After that, a calcination step not only made intimate contacts with two semiconductors, but also converted TNDs into TiO2 nanoparticles. Due to the position of conduction band edges of two semiconductors, photogenerated electrons could transfer from g-C3N4 to TiO2. There with a help of Pt as a cocatalyst and active sites provider, photoexcited electrons reduced protons from water and generated hydrogen. This heterojunction could produce more than double hydrogen as pristine g-C3N4 under the same conditions. We created a novel g-C3N4 nanosheets with carbon vacancies and nanoholes throughout nanosheet planes. After synthesis g-C3N4 bulk material from dicyandiamide, the obtained material was heated to 650 ºC under argon flow for 2 hr. After it cooled down, it was calcined again at 500 ºC for 2 hr. As a result, its specific surface area increased significantly from 28 m2 g-1 of bulk g-C3N4 to 160 m2 g-1. Moreover, these stepwise treatments introduced some defects as carbon vacancies inside the structure of g-C3N4 nanosheets. They provided highly active photocatalytic sites for hydrogen evolution. Therefore, its hydrogen production was ten times higher than bulk material of g-C3N4 under visible light irradiation. It showed very high quantum efficiencies of 29.2% and 21.3% at 400 nm and 420 nm, respectively. Finally, we generated zinc cadmium solid solution (ZnxCd1-xS) with synthesizing metal-glycerate of Cd and Zn via solvothermal method. Then, the material was calcined (500 ºC for 4 hr) and treated with H2S at 450 ºC for 2hr. Thus, an homogeneous solid solution of ZnxCd1-xS with hexagonal wurtzite crystal structure was formed. It should be mentioned that the obtained semiconductor could absorb a wide range of visible light energy and its band gap is strongly affected by Zn/Cd ratio and varies between 2.35 and 3.4 eV (0≤x≤1). The best results for hydrogen evolution was gained from Zn30Cd70S sample with depositing MoS2 as a cocatalyst. It could generate hydrogen in longer wavelengths of visible light region and its quantum efficiencies were: 46.6 % at 400 nm to 23.4% at 500 nm as well as 11.3% at 550 nm.

Molecular dynamics simulations were carried out on traditional polymers copolymerized with POSS (Polyhedral Oligomeric Silsesquioxanes) derivatives to identify the reason behind improved properties imparted to the conventional polymers with the chemical incorporation of POSS. Two classes of systems are used in the present study, namely the polystyrene and polymethyl methacrylate systems. Seven systems are studied in the polystyrene class. The effect of corner substituent groups of the POSS cage on the properties of the polymer nanocomposites was studied using the polystyrene. In addition, the effect of the type of cage structure on the properties was studied using T8, T10 and T12 POSS cage structures containing phenyl substituents on each POSS cage. Systems with polymethyl methacrylate were studied to analyze the effect of mole percent of POSS on the polymer properties, holding the corner substituents on the POSS unit constant. The corner function used was the isobutyl group. The properties analyzed using simulations include glass transition temperature, volumetric thermal expansion coefficient, X-ray scattering data, solubility parameter and mechanical properties. In both polystyrene and polymethyl methacrylate systems, simulations were also carried out on the pure parent polymers for the sake of comparison. The effect of forcefield on the predicted properties was studied using both COMPASS and PCFF forcefields. Performance analysis of the code used in the present simulation was done by analyzing the parallel run time of simulations involving pure atactic polystyrene.

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