985 resultados para Molecular orientation
Resumo:
L’électrofilage est une technique de mise en œuvre efficace et versatile qui permet la production de fibres continues d’un diamètre typique de quelques centaines de nanomètres à partir de l’application d’un haut voltage sur une solution concentrée de polymères enchevêtrés. L’évaporation extrêmement rapide du solvant et les forces d’élongation impliquées dans la formation de ces fibres leur confèrent des propriétés hors du commun et très intéressantes pour plusieurs types d’applications, mais dont on commence seulement à effleurer la surface. À cause de leur petite taille, ces matériaux ont longtemps été étudiés uniquement sous forme d’amas de milliers de fibres avec les techniques conventionnelles telles que la spectroscopie infrarouge ou la diffraction des rayons X. Nos connaissances de leur comportement proviennent donc toujours de la convolution des propriétés de l’amas de fibres et des caractéristiques spécifiques de chacune des fibres qui le compose. Les études récentes à l’échelle de la fibre individuelle ont mis en lumière des comportements inhabituels, particulièrement l’augmentation exponentielle du module avec la réduction du diamètre. L’orientation et, de manière plus générale, la structure moléculaire des fibres sont susceptibles d’être à l'origine de ces propriétés, mais d’une manière encore incomprise. L’établissement de relations structure/propriétés claires et l’identification des paramètres qui les influencent représentent des défis d’importance capitale en vue de tirer profit des caractéristiques très particulières des fibres électrofilées. Pour ce faire, il est nécessaire de développer des méthodes plus accessibles et permettant des analyses structurales rapides et approfondies sur une grande quantité de fibres individuelles présentant une large gamme de diamètre. Dans cette thèse, la spectroscopie Raman confocale est utilisée pour l’étude des caractéristiques structurales, telles que l’orientation moléculaire, la cristallinité et le désenchevêtrement, de fibres électrofilées individuelles. En premier lieu, une nouvelle méthodologie de quantification de l’orientation moléculaire par spectroscopie Raman est développée théoriquement dans le but de réduire la complexité expérimentale de la mesure, d’étendre la gamme de matériaux pour lesquels ces analyses sont possibles et d’éliminer les risques d’erreurs par rapport à la méthode conventionnelle. La validité et la portée de cette nouvelle méthode, appelée MPD, est ensuite démontrée expérimentalement. Par la suite, une méthodologie efficace permettant l’étude de caractéristiques structurales à l’échelle de la fibre individuelle par spectroscopie Raman est présentée en utilisant le poly(éthylène téréphtalate) comme système modèle. Les limites de la technique sont exposées et des stratégies expérimentales pour les contourner sont mises de l’avant. Les résultats révèlent une grande variabilité de l'orientation et de la conformation d'une fibre à l'autre, alors que le taux de cristallinité demeure systématiquement faible, démontrant l'importance et la pertinence des études statistiques de fibres individuelles. La présence de chaînes montrant un degré d’enchevêtrement plus faible dans les fibres électrofilées que dans la masse est ensuite démontrée expérimentalement pour la première fois par spectroscopie infrarouge sur des amas de fibres de polystyrène. Les conditions d'électrofilage favorisant ce phénomène structural, qui est soupçonné d’influencer grandement les propriétés des fibres, sont identifiées. Finalement, l’ensemble des méthodologies développées sont appliquées sur des fibres individuelles de polystyrène pour l’étude approfondie de l’orientation et du désenchevêtrement sur une large gamme de diamètres et pour une grande quantité de fibres. Cette dernière étude permet l’établissement de la première relation structure/propriétés de ces matériaux, à l’échelle individuelle, en montrant clairement le lien entre l’orientation moléculaire, le désenchevêtrement et le module d'élasticité des fibres.
Resumo:
L’électrofilage est une technique de mise en œuvre efficace et versatile qui permet la production de fibres continues d’un diamètre typique de quelques centaines de nanomètres à partir de l’application d’un haut voltage sur une solution concentrée de polymères enchevêtrés. L’évaporation extrêmement rapide du solvant et les forces d’élongation impliquées dans la formation de ces fibres leur confèrent des propriétés hors du commun et très intéressantes pour plusieurs types d’applications, mais dont on commence seulement à effleurer la surface. À cause de leur petite taille, ces matériaux ont longtemps été étudiés uniquement sous forme d’amas de milliers de fibres avec les techniques conventionnelles telles que la spectroscopie infrarouge ou la diffraction des rayons X. Nos connaissances de leur comportement proviennent donc toujours de la convolution des propriétés de l’amas de fibres et des caractéristiques spécifiques de chacune des fibres qui le compose. Les études récentes à l’échelle de la fibre individuelle ont mis en lumière des comportements inhabituels, particulièrement l’augmentation exponentielle du module avec la réduction du diamètre. L’orientation et, de manière plus générale, la structure moléculaire des fibres sont susceptibles d’être à l'origine de ces propriétés, mais d’une manière encore incomprise. L’établissement de relations structure/propriétés claires et l’identification des paramètres qui les influencent représentent des défis d’importance capitale en vue de tirer profit des caractéristiques très particulières des fibres électrofilées. Pour ce faire, il est nécessaire de développer des méthodes plus accessibles et permettant des analyses structurales rapides et approfondies sur une grande quantité de fibres individuelles présentant une large gamme de diamètre. Dans cette thèse, la spectroscopie Raman confocale est utilisée pour l’étude des caractéristiques structurales, telles que l’orientation moléculaire, la cristallinité et le désenchevêtrement, de fibres électrofilées individuelles. En premier lieu, une nouvelle méthodologie de quantification de l’orientation moléculaire par spectroscopie Raman est développée théoriquement dans le but de réduire la complexité expérimentale de la mesure, d’étendre la gamme de matériaux pour lesquels ces analyses sont possibles et d’éliminer les risques d’erreurs par rapport à la méthode conventionnelle. La validité et la portée de cette nouvelle méthode, appelée MPD, est ensuite démontrée expérimentalement. Par la suite, une méthodologie efficace permettant l’étude de caractéristiques structurales à l’échelle de la fibre individuelle par spectroscopie Raman est présentée en utilisant le poly(éthylène téréphtalate) comme système modèle. Les limites de la technique sont exposées et des stratégies expérimentales pour les contourner sont mises de l’avant. Les résultats révèlent une grande variabilité de l'orientation et de la conformation d'une fibre à l'autre, alors que le taux de cristallinité demeure systématiquement faible, démontrant l'importance et la pertinence des études statistiques de fibres individuelles. La présence de chaînes montrant un degré d’enchevêtrement plus faible dans les fibres électrofilées que dans la masse est ensuite démontrée expérimentalement pour la première fois par spectroscopie infrarouge sur des amas de fibres de polystyrène. Les conditions d'électrofilage favorisant ce phénomène structural, qui est soupçonné d’influencer grandement les propriétés des fibres, sont identifiées. Finalement, l’ensemble des méthodologies développées sont appliquées sur des fibres individuelles de polystyrène pour l’étude approfondie de l’orientation et du désenchevêtrement sur une large gamme de diamètres et pour une grande quantité de fibres. Cette dernière étude permet l’établissement de la première relation structure/propriétés de ces matériaux, à l’échelle individuelle, en montrant clairement le lien entre l’orientation moléculaire, le désenchevêtrement et le module d'élasticité des fibres.
Resumo:
Refractive index and structural characteristics of optical polymers are strongly influenced by the thermal history of the material. Polymer optical fibres (POF) are drawn under tension, resulting in axial orientation of the polymer molecular chains due to their susceptibility to align in the fibre direction. This change in orientation from the drawing process results in residual strain in the fibre and also affects the transparency and birefringence of the material (1-3). PMMA POF has failure strain as high as over 100%. POF has to be drawn under low tension to achieve this value. The drawing tension affects the magnitude of molecular alignment along the fibre axis, thus affecting the failure strain. The higher the tension the lower the failure stain will be. However, the properties of fibre drawn under high tension can approach that of fibre drawn under low tension by means of an annealing process. Annealing the fibre can generally optimise the performance of POF while keeping most advantages intact. Annealing procedures can reduce index difference throughout the bulk and also reduce residual stress that may cause fracture or distortion. POF can be annealed at temperatures approaching the glass transition temperature (Tg) of the polymer to produce FBG with a permanent blue Bragg wave-length shift at room temperature. At this elevated temperature segmental motion in the structure results in a lower viscosity. The material softens and the molecular chains relax from the axial orientation causing shrinking of the fibre. The large attenuation of typically 1dB/cm in the 1550nm spectral region of PMMA POF has limited FBG lengths to less than 10cm. The more expensive fluorinated polymers with lower absorption have had no success as FBG waveguides. Bragg grating have been inscribed onto various POF in the 800nm spectral region using a 30mW continuous wave 325nm helium cadmium laser, with a much reduced attenuation coefficient of 10dB/m (5). Fabricating multiplexed FBGs in the 800nm spectral region in TOPAS and PMMA POF consistently has lead to fabrication of multiplexed FBG in the 700nm spectral region by a method of prolonged annealing. The Bragg wavelength shift of gratings fabricated in PMMA fibre at 833nm and 867nm was monitored whilst the POF was thermally annealed at 80°C. Permanent shifts exceeding 80nm into the 700nm spectral region was attained by both gratings on the fibre. The large permanent shift creates the possibility of multiplexed Bragg sensors operating over a broad range. -------------------------------------------------------------------------------------------------------------------- 1. Pellerin C, Prud'homme RE, Pézolet M. Effect of thermal history on the molecular orientation in polystyrene/poly (vinyl methyl ether) blends. Polymer. 2003;44(11):3291-7. 2. Dvoránek L, Machová L, Šorm M, Pelzbauer Z, Švantner J, Kubánek V. Effects of drawing conditions on the properties of optical fibers made from polystyrene and poly (methyl methacrylate). Die Angewandte Makromolekulare Chemie. 1990;174(1):25-39. 3. Dugas J, Pierrejean I, Farenc J, Peichot JP. Birefringence and internal stress in polystyrene optical fibers. Applied optics. 1994;33(16):3545-8. 4. Jiang C, Kuzyk MG, Ding JL, Johns WE, Welker DJ. Fabrication and mechanical behavior of dye-doped polymer optical fiber. Journal of applied physics. 2002;92(1):4-12. 5. Johnson IP, Webb DJ, Kalli K, Yuan W, Stefani A, Nielsen K, et al., editors. Polymer PCF Bragg grating sensors based on poly (methyl methacrylate) and TOPAS cyclic olefin copolymer2011: SPIE.
Resumo:
Refractive index and structural characteristics of optical polymers are strongly influenced by the thermal history of the material. Polymer optical fibres (POF) are drawn under tension, resulting in axial orientation of the polymer molecular chains due to their susceptibility to align in the fibre direction. This change in orientation from the drawing process results in residual strain in the fibre and also affects the transparency and birefringence of the material (1-3). PMMA POF has failure strain as high as over 100%. POF has to be drawn under low tension to achieve this value. The drawing tension affects the magnitude of molecular alignment along the fibre axis, thus affecting the failure strain. The higher the tension the lower the failure stain will be. However, the properties of fibre drawn under high tension can approach that of fibre drawn under low tension by means of an annealing process. Annealing the fibre can generally optimise the performance of POF while keeping most advantages intact. Annealing procedures can reduce index difference throughout the bulk and also reduce residual stress that may cause fracture or distortion. POF can be annealed at temperatures approaching the glass transition temperature (Tg) of the polymer to produce FBG with a permanent blue Bragg wave-length shift at room temperature. At this elevated temperature segmental motion in the structure results in a lower viscosity. The material softens and the molecular chains relax from the axial orientation causing shrinking of the fibre. The large attenuation of typically 1dB/cm in the 1550nm spectral region of PMMA POF has limited FBG lengths to less than 10cm. The more expensive fluorinated polymers with lower absorption have had no success as FBG waveguides. Bragg grating have been inscribed onto various POF in the 800nm spectral region using a 30mW continuous wave 325nm helium cadmium laser, with a much reduced attenuation coefficient of 10dB/m (5). Fabricating multiplexed FBGs in the 800nm spectral region in TOPAS and PMMA POF consistently has lead to fabrication of multiplexed FBG in the 700nm spectral region by a method of prolonged annealing. The Bragg wavelength shift of gratings fabricated in PMMA fibre at 833nm and 867nm was monitored whilst the POF was thermally annealed at 80°C. Permanent shifts exceeding 80nm into the 700nm spectral region was attained by both gratings on the fibre. The large permanent shift creates the possibility of multiplexed Bragg sensors operating over a broad range. -------------------------------------------------------------------------------------------------------------------- 1. Pellerin C, Prud'homme RE, Pézolet M. Effect of thermal history on the molecular orientation in polystyrene/poly (vinyl methyl ether) blends. Polymer. 2003;44(11):3291-7. 2. Dvoránek L, Machová L, Šorm M, Pelzbauer Z, Švantner J, Kubánek V. Effects of drawing conditions on the properties of optical fibers made from polystyrene and poly (methyl methacrylate). Die Angewandte Makromolekulare Chemie. 1990;174(1):25-39. 3. Dugas J, Pierrejean I, Farenc J, Peichot JP. Birefringence and internal stress in polystyrene optical fibers. Applied optics. 1994;33(16):3545-8. 4. Jiang C, Kuzyk MG, Ding JL, Johns WE, Welker DJ. Fabrication and mechanical behavior of dye-doped polymer optical fiber. Journal of applied physics. 2002;92(1):4-12. 5. Johnson IP, Webb DJ, Kalli K, Yuan W, Stefani A, Nielsen K, et al., editors. Polymer PCF Bragg grating sensors based on poly (methyl methacrylate) and TOPAS cyclic olefin copolymer2011: SPIE.
Resumo:
The Bragg wavelength of a PMMA based fiber grating is determined by the effective core index and the grating pitch, which, in temperature sensing, depend on the thermo-optic and thermal expansion coefficients of PMMA. These two coefficients are a function of surrounding temperature and humidity. Amorphous polymers including PMMA exhibit a certain degree of anisotropic thermal expansion. The anisotropic nature of expansion mainly depends on the polymer processing history. The expansion coefficient is believed to be lower in the direction of the molecular orientation than in the direction perpendicular to the draw direction. Such anisotropic behavior of polymers can be expected in drawn PMMA based optical fiber, and will lead to a reduced thermal expansion coefficient and larger temperature sensitivity than would be the case were the fiber to be isotropic. Extensive work has been carried out to identify these factors. The temperature responses of gratings have been measured at different relative humidity. Gratings fabricated on annealed and non-annealed PMMA optical fibers are used to compare the sensitivity performance as annealing is considered to be able to mitigate the anisotropic effect in PMMA optical fiber. Furthermore an experiment has been designed to eliminate the thermal expansion contribution to the grating wavelength change, leading to increased temperature sensitivity and improved response linearity. © 2014 Copyright SPIE.
Resumo:
Organic-graphene system has emerged as a new platform for various applications such as flexible organic photovoltaics and organic light emitting diodes. Due to its important implication in charge transport, the study and reliable control of molecular packing structures at the graphene-molecule interface are of great importance for successful incorporation of graphene in related organic devices. Here, an ideal membrane of suspended graphene as a molecular assembly template is utilized to investigate thin-film epitaxial behaviors. Using transmission electron microscopy, two distinct molecular packing structures of pentacene on graphene are found. One observed packing structure is similar to the well-known bulk-phase, which adapts a face-on molecular orientation on graphene substrate. On the other hand, a rare polymorph of pentacene crystal, which shows significant strain along the c-axis, is identified. In particular, the strained film exhibits a specific molecular orientation and a strong azimuthal correlation with underlying graphene. Through ab initio electronic structure calculations, including van der Waals interactions, the unusual polymorph is attributed to the strong graphene-pentacene interaction. The observed strained organic film growth on graphene demonstrates the possibility to tune molecular packing via graphene-molecule interactions.
Resumo:
We have examined the effect of the uncharged species of lidocaine (LDC) and etidocaine (EDC) on the acyl chain moiety of egg phosphatidylcholine liposomes. Changes in membrane organization caused by both anesthetics were detected through the use of EPR spin labels (5, 7 and 12 doxyl stearic acid methyl ester) or fluorescence probes (4, 6, 10, 16 pyrene-fatty acids). The disturbance caused by the LA was greater when the probes were inserted in more external positions of the acyl chain and decreased towards the hydrophobic core of the membrane. The results indicate a preferential insertion of LDC at the polar interface of the bilayer and in the first half of the acyl chain, for EDC. Additionally, 2 H NMR spectra of multilamellar liposomes composed by acyl chain-perdeutero DMPC and EPC (1:4 mol%) allowed the determination of the segmental order (S-mol) and dynamics (T-1) of the acyl chain region. In accordance to the fluorescence and EPR results, changes in molecular orientation and dynamics are more prominent if the LA preferential location is more superficial, as for LDC while EDC seems to organize the acyl chain region between carbons 2-8, which is indicative of its positioning. We propose that the preferential location of LDC and EDC inside the bilayers creates a "transient site", which is related to the anesthetic potency since it could modulate the access of these molecules to their binding site(s) in the voltage-gated sodium channel. (C) 2007 Elsevier B.V. All rights reserved.
Resumo:
The thermal behavior of kaolinite–urea intercalation complex was investigated by thermogravimetry–differential scanning calorimetry (TG–DSC), X-ray diffraction (XRD), and fourier transform infrared spectroscopy (FTIR). In addition, the interaction mode of urea molecules intercalated into the kaolinite gallery was studied by means of molecular dynamics simulation. Three main mass losses were observed at 136 °C, in the range of 210–270 °C, and at 500 °C in the TG–DSC curves, which were, respectively, attributed to (1) melting of the surface-adsorbed urea, (2) removal of the intercalated urea, and (3) dehydroxylation of the deintercalated kaolinite. The three DSC endothermic peaks at 218, 250, and 261 °C were related to the successive removals of intercalated urea with three different distribution structures. Based on the angle between the dipole moment vector of urea and the basal surface of kaolinite, the three urea models could be described as follows: (1) Type A, the dipole moment vector is nearly parallel to the basal surface of kaolinite; (2) Type B, the dipole moment vector points to the silica tetrahedron with the angle between it and the basal surface of kaolinite ranging from 20°to 40°; and (3) Type C, the dipole moment vector is nearly perpendicular to the basal surface of kaolinite. The three distribution structures of urea molecules were validated by the results of the molecular dynamics simulation. Furthermore, the thermal behavior of the kaolinite–urea intercalation complex investigated by TG–DSC was also supported by FTIR and XRD analyses.
Resumo:
Surface orientation of self-assembled molecular films of 2,9,6,23-tetraamino cobalt phthalocyanine on gold and silver is shown to determine the nature and the products of the electrocatalytic reduction of oxygen.
Resumo:
In the present paper, thermo-mechanical response of B2-NiAl nanowire along the < 100 >, < 110 >, and < 111 > orientations has been studied using molecular dynamics simulations. Nanowire with cross-sectional dimensions of similar to 20x20 angstrom(2), similar to 25x25 angstrom(2), and similar to 30x30 angstrom(2) and temperature range of 10 K-900 K has been considered. A Combined effect of size, orientation, and temperature on the stress-strain behavior under uniaxial tensile loading has been presented. It has been observed that < 111 > oriented NiAl nanowire that is energetically most stable gives highest yield stress which further reduces with < 110 > and < 100 > orientations. A remarkable ductile brittle transition (DBT) with an increase in temperature has also been reported for all the orientations considered in the present study. The DBT observed for the nanowire has also been compared with the reported DBT of bulk B2-NiAl obtained from experiments. Alternate technique has also been proposed to increase the toughness of a given material especially at lower temperature regions, i.e. below DBT.
Influence of substrate orientation on In0.5Ga0.5As/GaAs quantum dots grown by molecular beam epitaxy
Resumo:
In this paper, In0.5Ga0.5As quantum dots are fabricated on GaAs (100) and (n11)A/B (n = 3, 5) substrates by molecular beam epitaxy. Atomic force microscopy shows that the quantum dots on each oriented substrate are different in size, shape and distribution. In addition, photoluminescence spectra from these quantum dots are different in emission peak position, line width and integrated intensity. Auger electron spectra demonstrate that In concentration is larger near the surface than inside quantum dots, suggesting the occurrence of surface segregation effect during the growth of InGaAs dots. The surface segregation effect is found to be related to substrate orientation. (C) 2000 Elsevier Science B.V. All rights reserved.
Influence of substrate orientation on In0.5Ga0.5As/GaAs quantum dots grown by molecular beam epitaxy
Resumo:
In this paper, In0.5Ga0.5As quantum dots are fabricated on GaAs (100) and (n11)A/B (n = 3, 5) substrates by molecular beam epitaxy. Atomic force microscopy shows that the quantum dots on each oriented substrate are different in size, shape and distribution. In addition, photoluminescence spectra from these quantum dots are different in emission peak position, line width and integrated intensity. Auger electron spectra demonstrate that In concentration is larger near the surface than inside quantum dots, suggesting the occurrence of surface segregation effect during the growth of InGaAs dots. The surface segregation effect is found to be related to substrate orientation. (C) 2000 Elsevier Science B.V. All rights reserved.
Resumo:
The molecular chain and lamellar crystal orientation in ultrathin films (thickness < 100 nm) of poly(di-n-hexylsilane) (PDHS) on silicon wafer substrates have been investigated by using transmission electronic microscopy, wide-angle X-ray diffraction, atomic force microscopy, and UV absorption spectroscopy. PDHS showed a film thickness-dependent molecular chain and lamellar crystal orientation. Lamellar crystals grew preferentially in flat-on orientation in the monolayer ultrathin films of PDHS, i.e., the silicon backbones were oriented along the surface-normal direction. By contrast, the orientation of lamellar crystals was preferentially edge-on in ultrathin films thicker than ca. 13 nm, i.e., the silicon backbones were oriented parallel to the substrate surface. We interpret the different orientations of molecular chain and lamellar crystal as due to the reduction of the entropy of the polymer chain near the substrate surface and the particularity of the crystallographic (001) plane of flat-on lamellae, respectively. A remarkable influence of the orientations of the silicon backbone on the UV absorption of these PDHS ultrathin films was observed due to the one-dimensional nature of sigma-electrons delocalized along the silicon backbone.
Resumo:
High resolution friction force maps of the benzylammonium terminated crystalline surface of a layer compound are presented. The lateral force map acquired with an atomic force microscope, reveals a significant contrast between different molecular orientations yielding molecular rows which differ from their neighboring ones. The single crystals are formed by stacks of copper oxalate sheets sandwiched between stereoregular organic cations, resulting in highly organized surface structures. Single molecular defects are observed at small loads. The experimental results are compared with numerical calculations which indicate a transition from an unperturbed state at small loads to a distorted state at higher loads. (C) 2011 American Institute of Physics.