Dissertations / Theses on the topic 'Lower critical solution temperature'

Poly(N-vinylcaprolactam), PNVCL, is a nonionic, nontoxic, water soluble, thermally sensitive and biocompatible polymer. It contains hydrophilic carboxylic and amide groups with hydrophobic carbon-carbon backbone chain so its hydrolysis does not produce small amide compounds which are often not desired for biomedical applications. Moreover PNVCL possesses lower critical solution temperature, (LCST) in the range of physiological temperature (32-34 oC). These properties make the polymer suitable for use in some biotechnology applications such as implantation of artificial organs and tissues, purification of enzymes, proteins and living cells, and in drug release systems. In this study PNVCL was synthesized by free radical polymerization with solution technique. Polymerization was done at different temperatures for different time periods in an oil bath. The activation energy for polymerization was found from Arrhenius plot as 108.4 kJ/mol. Polymer was characterized by FT-IR, 1H-NMR and 13C-NMR, DSC, TGA and XRD techniques. FT-IR and NMR measurements confirmed that the polymerization proceeded through the vinyl group.

The overall aim of my PhD research was to develop biocompatible materials, namely poly(2-oxazoline)s, in terms of chemical structures and chemical and physical properties for drug delivery systems. This thesis demonstrated novel strategies and unique approaches towards sophisticated drug delivery formulations. A combination of crosslinking chemistry, thermoresponsive properties, and drug conjugation was introduced to overcome common issues in typical drug delivery devices such as burst drug release and low drug efficiency. Ultimately, this thesis aimed to promote poly(2-oxazoline)s as the most promising emerging polymers in the future.

R??sum?? : Les copolym??res ?? blocs sensibles aux stimuli (SR-BCPs) et leurs assemblages, tels que les micelles, les v??sicules et les hydrogels, peuvent subir des changements physiques ou chimiques en r??ponse ?? l'??volution des conditions environnementales. Pour un excellent SR-BCP, habituellement, de l??g??res modifications de l'environnement sont suffisantes pour induire des modifications relativement drastiques dans la conformation, la structure ou les propri??t??s du polym??re. Ces polym??res sont aussi appel??s polym??res stimuli-r??actifs ou polym??res intelligents et ils ont un grand potentiel d'application dans de nombreux domaines. Au cours des deux derni??res d??cennies, un int??r??t de recherche et d??veloppement particulier a ??t?? port?? sur l'exploitation des SR-BCPs pour utilisation comme syst??mes de relargage de m??dicaments. Dans de nombreux cas, les changements induits par des stimuli dans la structure ou la morphologie des assemblages de BCPs peuvent entra??ner la lib??ration de l'esp??ce encapsul??e, parfois d'une mani??re contr??lable spatialement et temporellement par le choix d'un stimulus appropri?? et en ajustant les param??tres de la m??thode de stimulation utilis??e. De fa??on g??n??rale, le fait d???avoir un certain type de groupements r??actifs ?? un stimulus donn?? dans la structure permet aux SR-BCPs de reconna??tre et r??agir ?? ce stimulus. Malgr?? les ??normes progr??s r??alis??s sur les SR-BCPs, un certain nombre de questions fondamentales restent ?? r??soudre afin de leur permettre de se trouver dans des applications pratiques. Pour y arriver, la cl?? ou le d??fi r??side dans l???am??lioration du niveau et de la complexit?? de contr??le sur les SR-BCPs ainsi que la sensibilit?? avec laquelle ces polym??res r??agissent ?? des stimuli. G??n??ralement, il est souhaitable d'obtenir une r??action rapide sous l'action d'une stimulation mod??r??e. A cette fin, il est n??cessaire d???effectuer des recherches fondamentales sur la conception rationnelle de nouveaux SR-BCPs ainsi que sur le d??veloppement de m??thodes de stimulation qui peuvent amplifier l'effet d'un stimulus. Les travaux de recherche pr??sent??s dans cette th??se s'inscrivent dans ce domaine de recherche. Plus sp??cifiquement, nous avons ??tudi?? des micelles de BCPs qui r??pondent ?? deux types de stimuli. D'une part, nous avons ??tudi?? un m??canisme d'amplification bas?? sur l???effet des ultrasons combin?? ?? la thermosensibilit?? de BCPs. D'autre part, nous avons d??velopp?? une nouvelle conception de BCPs qui permet aux micelles d?????tre d??truites soit de mani??re photochimique, soit par des r??actions d'oxydo-r??duction, tout en ayant le nombre minimum des groupes stimuli-r??actifs dans la structure du polym??re. Notre recherche a g??n??r?? de nouvelles connaissances dans ce domaine et sugg??re de nouveaux moyens sur la fa??on dont les questions de sensibilit?? et de contr??le complexe des micelles SR-BCPs peuvent ??tre abord??es, contribuant ainsi ?? l'avancement des connaissances fondamentales. Le c??ur de cette th??se est compos?? de trois publications r??sultant des projets r??alis??s. Dans le premier projet, afin de coupler la sensibilit?? aux ultrasons et la thermosensibilit??, nous avons men?? une ??tude ayant pour but de trouver des structures possibles de polym??res qui sont susceptibles d'??tre affect??es par les ultrasons. Nous avons effectu?? une ??tude comparative sur la destruction des micelles form??es par divers BCPs et la lib??ration concomitante d'un colorant hydrophobe encapsul?? (rouge du Nil) par les ultrasons focalis??s de haute intensit?? (HIFU). Nous avons constat?? que toutes les micelles form??es par les quatre copolym??res diblocs synth??tis??s, ??tant constitu??s d'un m??me bloc du polyoxyde d'??thyl??ne (PEO) hydrophile et d???un bloc de polym??thacrylate hydrophobe diff??rent, peuvent ??tre perturb??es par les ultrasons. Toutefois, l'ampleur de la perturbation et la lib??ration du colorant encapsul?? dans la micelle est influenc??e par la structure chimique du block hydrophobe. En particulier, les micelles du PEO-b-PIBMA (poly(1-isobutoxym??thacrylate d'??thyle)) et du PEO-b-PTHPMA (poly(m??thacrylate de 2-t??trahydropyrannyle)), qui poss??dent une unit?? ac??tal labile dans le groupe lat??ral, subissent des perturbations plus importantes en raison, probablement, d???une r??action d???hydrolyse de l???ester induite par les ultrasons, donnant lieu ?? une lib??ration plus rapide du colorant. En revanche, les micelles du PEO-b-PMMA (poly(m??thacrylate de m??thyle)), dont le bloc polym??thacrylate est plus stable, sont plus r??sistantes aux ultrasons et pr??sentent une cin??tique de lib??ration du colorant plus lente que les autres micelles. De plus, l???analyse des spectres infrarouges des solutions micellaires, enregistr??s avant et apr??s l???exposition aux ultrasons, sugg??re une r??action d???hydrolyses pour le PEO-b-PIBMA et le PEO-b-PTHPMA, mais montre l'absence d???une quelconque r??action chimique pour le PEO-b-PMMA. L'effet de la structure de copolym??re ?? blocs sur la r??activit?? des micelles ?? l'irradiation HIFU ?? hautes fr??quences permet de mieux comprendre comment des micelles de BCPs sensibles aux ultrasons peuvent ??tre con??ues. Sur la base du premier projet, dans le deuxi??me projet, nous avons d??montr?? une nouvelle approche pouvant amplifier l'effet de HIFU sur la destruction des micelles de BCPs en solution aqueuse. L???id??e est d???introduire une petite quantit?? des unit??s comonom??res sensibles aux ultrasons dans le bloc thermosensible et initialement hydrophobe. On peut alors former une micelle dont le noyau est compos?? du polym??re sensible aux ultrasons. Si la r??action induite par les ultrasons sur le noyau permet d???augmenter la temp??rature de solution critique inf??rieure (LCST) du polym??re thermosensible au-dessus de la temp??rature de la solution micellaire, la micelle doit ??tre dissolue car tout le BCP est devenu soluble dans l???eau. Pour tester la validit?? de ce nouveau m??canisme, nous avons synth??tis?? et ??tudi?? un copolym??re dibloc de PEO-b-P(MEO[indice inf??rieur 2]MA-co-THPMA) (MEO[indice inf??rieur 2]MA repr??sente 2-(2-m??thoxy??thoxy) m??thacrylate d'??thyle), dans lequel le bloc thermosensible P(MEO[indice inf??rieur 2]MA-co-THPMA) est hydrophobe ?? T>LCST. Le THPMA a ??t?? choisi en raison de sa plus grande r??activit?? vis-??-vis des faisceaux HIFU que les autres monom??res ??tudi??s dans le premier projet. Les r??sultats montrent que les HIFU peuvent effectivement augmenter la LCST du bloc P(MEO[indice inf??rieur 2]MA-co-THPMA) et, par cons??quent, induire la dissociation des micelles ?? une temp??rature constante de la solution. Une analyse spectrale en RMN [indice sup??rieur 13]C a fourni des preuves montrant que l'hydrolyse des groupes THPMA se produit sous l???irradiation HIFU et que la destruction des micelles provient d'une augmentation de la LCST en raison de la conversion des motifs hydrophobes THPMA en motifs acides m??thacryliques (MAA) hydrophiles. Cette m??thode de modifier la LCST par une irradiation des ultrasons est g??n??rale et peut ??tre appliqu??e aux autres groupements sensibles aux ultrasons dans la conception de ce type de SR-BCPs. Cette ??tude a ainsi d??montr?? un nouveau m??canisme d'amplification et de contr??le des micelles de BCPs via la modification induite par les ultrasons de la temp??rature de transition de phase (LCST) du bloc constituant le noyau micellaire. Le troisi??me projet pr??sent?? dans cette th??se portait sur une conception rationnelle de BCPs ayant un but pr??cis: permettre aux micelles d?????tre perturb??es par deux types de stimuli en utilisant le nombre minimal des unit??s sensibles ?? des stimuli dans la structure de BCPs. Pour ce faire, nous avons con??u et synth??tis?? un nouveau copolym??re tribloc amphiphile de type ABC, soit le poly(oxyde d'??thyl??ne) - disulfure ??? polystyrene - o-nitrobenzyle - poly(2-(dim??thylamino) ??thylm??thacrylate) (PEO-S-S-PS-ONB-PDMAEMA). Il dispose d'une liaison disulfure redox-clivable entre les blocs PEO et PS ainsi que d'un groupe o-nitrobenzyle (ONB) photoclivable ?? la jonction des blocs PS et PDMAEMA. Nous avons montr?? que ce mod??le est une strat??gie utile pour permettre aux micelles de BCPs de r??pondre soit ?? un agent r??ducteur comme le dithiothr??itol (DTT) dans une solution, soit ?? l'exposition ?? la lumi??re UV, tout en ayant le nombre minimum des groups stimuli-r??actifs dans la structure du copolym??re (deux unit??s par cha??ne). Nos investigations ont r??v??l?? que les micelles de ce copolym??re tribloc peuvent ??tre perturb??es de diff??rentes fa??ons. Lorsqu'un seul stimulus est appliqu??, l'enl??vement d'un type des cha??nes de polym??re hydrophile ?? partir de la couronne de micelles, soit le PEO par clivage par oxydo-r??duction ou le PDMAEMA par photoclivage, entra??ne un effet limit?? de d??stabilisation sur la dispersion des micelles. L'agglom??ration de quelques micelles appara??t mais la dispersion reste essentiellement stable. En revanche, en cas d'utilisation combin??e des deux stimuli qui clivent ?? la fois le PEO et le PDMAEMA, une agr??gation importante du polym??re se produit ?? la suite de l'??limination de l'amphiphilicit?? du polym??re. // Abstract : Stimuli-responsive block copolymers (SR-BCPs) and their assemblies, such as micelles, vesicles and hydrogels, can undergo physical or chemical changes in response to changing environmental conditions. For an excellent SR-BCP, usually, slight changes in the environment are sufficient to induce relatively drastic changes in either the conformation or structure or properties of the polymer. Stimuli-reactive polymers are often referred to as smart polymers and they have great application potential in many fields. Over the past two decades, particular research and development interest has been focused on exploiting SR-BCP assemblies as drug delivery systems (DDSs). In many cases, stimuli-induced changes in the structure or morphology of BCP assemblies (drug carriers) can result in the release of loaded species, sometimes in a spatially and temporally controllable manner by choosing an appropriate stimulus and adjusting the parameters of the used stimulating method. Generally speaking, by having a certain type of stimuli-reactive moieties in the structure, SR-BCP assemblies have an ability to recognize a specific stimulus and react to its presence accordingly. Despite the tremendous progress achieved on SR-BCPs, a number of fundamental issues remain to be addressed in order to enable real-life applications of these smart polymers. Of them, an increasing level and complexity of control on SR-BCPs as well as the sensitivity with which these polymers react to stimuli are key and challenging. It is highly desirable to obtain a fast reaction under the action of a modest stimulation. To this end, fundamental research is necessary on rational and creative BCP structural design as well as on development of stimulation methods that can amplify the effect of a stimulus. The research work presented in this thesis falls into this important topic. More specifically, we studied BCP micelles that are responsive to two types of stimuli. On the one hand, we investigated an amplification mechanism based on coupling the ultrasound reactivity with the thermosensitivity of BCPs. On the other hand, we developed a BCP structural design that allows micelles to be disrupted by either light or redox agents while having the minimum number of stimuli-reactive moieties in the polymer structure. Our research provided new insights into and suggested new means on how the issues of sensitivity and complex control of SR-BCP micelles can be tackled, thus contributing to the advancement of fundamental knowledge. The core of this thesis is comprised of three publications resulting from the projects realized in our research work. In order to couple the ultrasound sensitivity and thermosensitivity, in the first project, we carried out studies to find possible polymer structures that are susceptible to be affected by ultrasound. We conducted a comparative study on the disruption of the micelles formed by various BCPs and the concomitant release of an encapsulated hydrophobic dye (Nile Red) by high-intensity focused ultrasound (HIFU). It was found that all micelles formed by the four synthesized diblock copolymers, being composed of a hydrophilic poly(ethylene oxide) (PEO) block and a different polymethacrylate hydrophobic block, could be disrupted by ultrasound. However, the extent of the micellar disruption and dye release was found to be influenced by the chemical structure of the micelle-core-forming hydrophobic polymethacrylate. In particular, micelles of PEO-b-PIBMA (poly(1-(isobutoxy)ethyl methacrylate)) and PEO-b-PTHPMA (poly(2-tetrahydropyranyl methacrylate)), whose hydrophobic blocks have a labile acetal unit in the side group and are more likely to undergo ester hydrolysis, could be disrupted more severely by ultrasound, giving rise to a faster release of Nile Red. By contrast, micelles of PEO-b-PMMA (poly(methyl methacrylate)), whose polymethacrylate block is more stable, appear to be more resistant to ultrasound irradiation and exhibit a slower rate of dye release than other BCPs. Moreover, infrared spectra recorded with micelles before and after ultrasound irradiation of the aqueous solution of the micelles give evidence for the occurrence of chemical reactions, most likely hydrolysis, for PEO-b-PIBMA and PEO-b-PTHPMA, but absence of chemical reactions for PEO-b-PMMA. The effect of BCP chemical structure on the reaction of micelles to high-frequency HIFU irradiation shows the perspective of designing and developing ultrasound-sensitive BCP micelles for ultrasound-based delivery applications. On the basis of the first project, in the second project, we demonstrated a new approach that could amplify the effect of HIFU on the disassembly of BCP micelles in aqueous solution. By introducing a small amount of ultrasound-labile comonomer units into the micelle core-forming thermosensitive polymer, the ultrasound-induced reaction of the comonomer could increase the lower critical solution temperature (LCST) of the thermosensitive polymer due to a polarity change, which renders the BCP soluble in water without changing the solution temperature and, consequently, results in disassembly of BCP micelles. To prove the validity of this new mechanism, we synthesized and investigated a diblock copolymer of PEO-b-P(MEO[subscript 2]MA-co-THPMA) (MEO[subscript 2]MA stands for 2-(2-methoxyethoxy)ethyl methacrylate). In the thermosensitive random copolymer block P(MEO[subscript 2]MA-co-THPMA), which is hydrophobic at T>LCST, THPMA was chosen due to its greater reactivity under HIFU than other monomer structures investigated in the first project. We found that HIFU could indeed increase the LCST of the P(MEO[subscript 2]MA-co-THPMA) block and, as a result, dissociate the BCP micelles at a constant temperature. A [superscript 13]C NMR spectral analysis provided critical evidence that hydrolysis of the THPMA groups occurs under HIFU irradiation and the micellar disassembly originates from an increase in the LCST due to the ultrasound-induced conversion of hydrophobic comonomer units of THPMA onto hydrophilic methacrylic acid (MAA). This ultrasound-changeable-LCST approach is general and can be applied by exploring other ultrasound-labile moieties in the BCP design. By transducing an ultrasound-induced effect into a changing thermosensitivity of the micelle core-forming block, this study demonstrated a new amplification and control mechanism for SR-BCP micelles. The third project presented in this thesis dealt with a rational BCP design that had a specific purpose: allowing BCP micelles to be disrupted by two types of stimuli while using the minimum number of stimuli-reactive moieties in the BCP structure. The unveiling of such BCP structures provides insight into how to make BCP micelles sensitive to stimuli. To do this, we designed and synthesized a new amphiphilic ABC-type triblock copolymer, namely, poly(ethylene oxide)-disulfide-polystyrene- o-nitrobenzyl-poly(2-(dimethylamino)ethylmethacrylate) (PEO-S-S-PS-ONB-PDMAEMA), which features a redox-cleavable disulfide linkage between the PEO and PS blocks as well as a photocleavable ONB group as the junction of the PS and PDMAEMA blocks. We demonstrated that this design is a useful strategy to allow BCP micelles to respond to both a reducing agent like dithiothreitol (DTT) in solution and exposure to UV light while having the minimum number of stimuli-reactive moieties in the block copolymer structure (two units per chain). Our investigations found that the micelles of this triblock copolymer could be disrupted in different ways. When only one stimulus is applied, the removal of one type of hydrophilic polymer chains from the micelle corona, either PEO by redox-cleavage or PDMAEMA by photocleavage, results in a limited destabilization effect on the dispersion of the micelles. The agglomeration between a few micelles appears but the dispersion remains essentially stable. By contrast, under combined use of the two stimuli that cleaves both PEO and PDMAEMA, severe polymer aggregation occurs as a result of elimination of the polymer amphiphilicity. Moreover, by loading the hydrophobic Nile Red in the micelles, the fluorescence quenching of the dye by aqueous medium under the different uses of the two stimuli appears to correlate with the different extents of the micellar disruption. // ?????? : ??????????????????????????????SR-BCPs???????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????SR-BCP???????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????-??????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????SR-BCP?????????????????????????????????DDSs???????????????????????????????????????BCP?????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????-????????????????????????SR-BCP??????????????????????????????????????????????????????????????????????????? ??????SR-BCPs?????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????SR-BCPs?????????????????????????????????????????????????????????????????????SR-BCPs???????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????BCP???????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????BCP???????????????????????????BCPs???????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????-???????????????BCP???????????????????????????????????????????????????????????????????????????????????????SR-BCP???????????????????????????????????????????????????????????????????????????????????????????????????????????? ??????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????BCPs????????????????????????????????????????????????HIFU?????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????PEO-b-PIBMA????????? 1-????????????????????????????????????????????? ??????PEO-b-PTHPMA?????????2-???????????????????????????????????? ??????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????? ??????????????????????????????????????????????????????????????????PEO-b-PMMA?????????????????????????????????????????????????????????????????????????????????????????????????????????PEO-b-PMMA????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????PEO-b-PIBMA???PEO-b-PTHPMA????????????????????????????????????????????????PEO-b-PMMA???????????????????????????????????????HIFU????????????BCP???????????????????????????????????????????????????????????????????????????-??????BCP????????????????????? ??????????????????????????????????????????????????????????????????????????????????????????????????????HIFU??????????????????BCP???????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????LCST?????????????????????????????????????????????????????????BCP??????????????????????????????BCP??????????????????????????????????????????????????????????????????????????????????????????????????????PEO-b-P(MEO2MA-co-THPMA) ???MEO2MA ??????2-???2-??????????????????????????????????????????????????????T > LCST????????????????????????????????????P(MEO2MA-co-THPMA)?????????????????????THPMA?????????????????????????????????????????????????????????????????????????????????HIFU?????????????????????????????????????????????????????????????????? ??????HIFU???????????????????????????P(MEO2MA-co-THPMA)?????????LCST?????????BCP??????????????????????????????????????????13C NMR ???????????????????????????THPMA?????????????????????????????????????????????THPMA??????????????????????????????MAA?????????LCST?????????????????????????????????????????????????????????????????????LCST??????????????????????????????????????????????????????BCP???????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????SR-BCP????????????????????????????????? ????????????????????????????????????????????????????????????????????????????????????????????????BCP????????????????????????????????????????????????????????????????????????BCP?????????????????????????????????????????????BCP?????????????????????????????????????????????????????????BCP????????????????????????????????????????????????????????????????????????ABC???????????????????????????????????????????????? - ???????????? - ???????????? - ??? - ???????????? - ?????? 2 - ???????????????????????????????????????????????? (PEO-S-S-PS-ONB-PDMAEMA)?????????PEO???PS???????????????????????????????????????????????????PS???PDMAEMA?????????????????????????????????ONB????????????????????????????????????????????????????????????-??????????????????????????????????????????????????????BCP????????????????????????????????????????????? ???DDT????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????PEO????????????????????????PDMAEMA?????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????PEO???PDMAEMA?????????????????????????????????????????????????????????????????????????????????????????????????????? ????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????????

Les solvants eutectiques profonds (DES) forment une nouvelle famille de solvants qui a émergé ces dernières années. Les DES sont de plus en plus étudiés de par leur faible coût, leur faible toxicité et leurs propriétés qui devraient leur permettre de remplacer des solvants toxiques utilisés dans de nombreux domaines de la chimie. Lors de ma thèse, un premier travail a permis d’établir les diagrammes de phases solide-liquide de trois DES partiellement biosourcés. Par la suite, une comparaison entre ces DES et des mélanges idéaux a permis d’établir que ces systèmes peuvent être considérés comme solvants eutectiques « profonds ». Au cours de mes travaux, un premier solvant aqueux possédant une température de solution critique inférieure a été mis en évidence et l’origine de cette propriété remarquable a été élucidée. Au-delà des travaux sur la compréhension des DES, ces solvants ont été testés pour deux applications : le captage du dioxyde de carbone et l’extraction liquide-liquide de colorants
Deep Eutectics Solvents (DES) is a new class of solvent which has emerged during the last decades. DES have been increasingly studied because of their low cost and low toxicity. Because of these properties, DES could potentially replace toxic solvents used in large area of chemistry. To reach this goal, a broader knowledge of these new systems has to be acquired. Therefore, in the first work of this thesis, solid-liquid phase diagrams of three partially renewable DES have been established. The comparison of these diagrams to an ideal mixing model is showing a negative deviation that allows to considered them as “deep” eutectics solvents. Following this work on the binary mixture, water was added to these DES. A first aqueous - DES mixture with a lower critical solution temperature (LSCT) has been highlighted and the origin of this remarkable property has been elucidated. To complete the initial work aiming to get a deeper understanding of these new DES, these solvents have also been tested for two applications: carbon dioxide capture and liquid-liquid extractions of dyes

Résumé : Les copolymères à blocs sensibles aux stimuli (SR-BCPs) et leurs assemblages, tels que les micelles, les vésicules et les hydrogels, peuvent subir des changements physiques ou chimiques en réponse à l'évolution des conditions environnementales. Pour un excellent SR-BCP, habituellement, de légères modifications de l'environnement sont suffisantes pour induire des modifications relativement drastiques dans la conformation, la structure ou les propriétés du polymère. Ces polymères sont aussi appelés polymères stimuli-réactifs ou polymères intelligents et ils ont un grand potentiel d'application dans de nombreux domaines. Au cours des deux dernières décennies, un intérêt de recherche et développement particulier a été porté sur l'exploitation des SR-BCPs pour utilisation comme systèmes de relargage de médicaments. Dans de nombreux cas, les changements induits par des stimuli dans la structure ou la morphologie des assemblages de BCPs peuvent entraîner la libération de l'espèce encapsulée, parfois d'une manière contrôlable spatialement et temporellement par le choix d'un stimulus approprié et en ajustant les paramètres de la méthode de stimulation utilisée. De façon générale, le fait d’avoir un certain type de groupements réactifs à un stimulus donné dans la structure permet aux SR-BCPs de reconnaître et réagir à ce stimulus. Malgré les énormes progrès réalisés sur les SR-BCPs, un certain nombre de questions fondamentales restent à résoudre afin de leur permettre de se trouver dans des applications pratiques. Pour y arriver, la clé ou le défi réside dans l’amélioration du niveau et de la complexité de contrôle sur les SR-BCPs ainsi que la sensibilité avec laquelle ces polymères réagissent à des stimuli. Généralement, il est souhaitable d'obtenir une réaction rapide sous l'action d'une stimulation modérée. A cette fin, il est nécessaire d’effectuer des recherches fondamentales sur la conception rationnelle de nouveaux SR-BCPs ainsi que sur le développement de méthodes de stimulation qui peuvent amplifier l'effet d'un stimulus. Les travaux de recherche présentés dans cette thèse s'inscrivent dans ce domaine de recherche. Plus spécifiquement, nous avons étudié des micelles de BCPs qui répondent à deux types de stimuli. D'une part, nous avons étudié un mécanisme d'amplification basé sur l’effet des ultrasons combiné à la thermosensibilité de BCPs. D'autre part, nous avons développé une nouvelle conception de BCPs qui permet aux micelles d’être détruites soit de manière photochimique, soit par des réactions d'oxydo-réduction, tout en ayant le nombre minimum des groupes stimuli-réactifs dans la structure du polymère. Notre recherche a généré de nouvelles connaissances dans ce domaine et suggère de nouveaux moyens sur la façon dont les questions de sensibilité et de contrôle complexe des micelles SR-BCPs peuvent être abordées, contribuant ainsi à l'avancement des connaissances fondamentales. Le cœur de cette thèse est composé de trois publications résultant des projets réalisés. Dans le premier projet, afin de coupler la sensibilité aux ultrasons et la thermosensibilité, nous avons mené une étude ayant pour but de trouver des structures possibles de polymères qui sont susceptibles d'être affectées par les ultrasons. Nous avons effectué une étude comparative sur la destruction des micelles formées par divers BCPs et la libération concomitante d'un colorant hydrophobe encapsulé (rouge du Nil) par les ultrasons focalisés de haute intensité (HIFU). Nous avons constaté que toutes les micelles formées par les quatre copolymères diblocs synthétisés, étant constitués d'un même bloc du polyoxyde d'éthylène (PEO) hydrophile et d’un bloc de polyméthacrylate hydrophobe différent, peuvent être perturbées par les ultrasons. Toutefois, l'ampleur de la perturbation et la libération du colorant encapsulé dans la micelle est influencée par la structure chimique du block hydrophobe. En particulier, les micelles du PEO-b-PIBMA (poly(1-isobutoxyméthacrylate d'éthyle)) et du PEO-b-PTHPMA (poly(méthacrylate de 2-tétrahydropyrannyle)), qui possèdent une unité acétal labile dans le groupe latéral, subissent des perturbations plus importantes en raison, probablement, d’une réaction d’hydrolyse de l’ester induite par les ultrasons, donnant lieu à une libération plus rapide du colorant. En revanche, les micelles du PEO-b-PMMA (poly(méthacrylate de méthyle)), dont le bloc polyméthacrylate est plus stable, sont plus résistantes aux ultrasons et présentent une cinétique de libération du colorant plus lente que les autres micelles. De plus, l’analyse des spectres infrarouges des solutions micellaires, enregistrés avant et après l’exposition aux ultrasons, suggère une réaction d’hydrolyses pour le PEO-b-PIBMA et le PEO-b-PTHPMA, mais montre l'absence d’une quelconque réaction chimique pour le PEO-b-PMMA. L'effet de la structure de copolymère à blocs sur la réactivité des micelles à l'irradiation HIFU à hautes fréquences permet de mieux comprendre comment des micelles de BCPs sensibles aux ultrasons peuvent être conçues. Sur la base du premier projet, dans le deuxième projet, nous avons démontré une nouvelle approche pouvant amplifier l'effet de HIFU sur la destruction des micelles de BCPs en solution aqueuse. L’idée est d’introduire une petite quantité des unités comonomères sensibles aux ultrasons dans le bloc thermosensible et initialement hydrophobe. On peut alors former une micelle dont le noyau est composé du polymère sensible aux ultrasons. Si la réaction induite par les ultrasons sur le noyau permet d’augmenter la température de solution critique inférieure (LCST) du polymère thermosensible au-dessus de la température de la solution micellaire, la micelle doit être dissolue car tout le BCP est devenu soluble dans l’eau. Pour tester la validité de ce nouveau mécanisme, nous avons synthétisé et étudié un copolymère dibloc de PEO-b-P(MEO[indice inférieur 2]MA-co-THPMA) (MEO[indice inférieur 2]MA représente 2-(2-méthoxyéthoxy) méthacrylate d'éthyle), dans lequel le bloc thermosensible P(MEO[indice inférieur 2]MA-co-THPMA) est hydrophobe à T>LCST. Le THPMA a été choisi en raison de sa plus grande réactivité vis-à-vis des faisceaux HIFU que les autres monomères étudiés dans le premier projet. Les résultats montrent que les HIFU peuvent effectivement augmenter la LCST du bloc P(MEO[indice inférieur 2]MA-co-THPMA) et, par conséquent, induire la dissociation des micelles à une température constante de la solution. Une analyse spectrale en RMN [indice supérieur 13]C a fourni des preuves montrant que l'hydrolyse des groupes THPMA se produit sous l’irradiation HIFU et que la destruction des micelles provient d'une augmentation de la LCST en raison de la conversion des motifs hydrophobes THPMA en motifs acides méthacryliques (MAA) hydrophiles. Cette méthode de modifier la LCST par une irradiation des ultrasons est générale et peut être appliquée aux autres groupements sensibles aux ultrasons dans la conception de ce type de SR-BCPs. Cette étude a ainsi démontré un nouveau mécanisme d'amplification et de contrôle des micelles de BCPs via la modification induite par les ultrasons de la température de transition de phase (LCST) du bloc constituant le noyau micellaire. Le troisième projet présenté dans cette thèse portait sur une conception rationnelle de BCPs ayant un but précis: permettre aux micelles d’être perturbées par deux types de stimuli en utilisant le nombre minimal des unités sensibles à des stimuli dans la structure de BCPs. Pour ce faire, nous avons conçu et synthétisé un nouveau copolymère tribloc amphiphile de type ABC, soit le poly(oxyde d'éthylène) - disulfure – polystyrene - o-nitrobenzyle - poly(2-(diméthylamino) éthylméthacrylate) (PEO-S-S-PS-ONB-PDMAEMA). Il dispose d'une liaison disulfure redox-clivable entre les blocs PEO et PS ainsi que d'un groupe o-nitrobenzyle (ONB) photoclivable à la jonction des blocs PS et PDMAEMA. Nous avons montré que ce modèle est une stratégie utile pour permettre aux micelles de BCPs de répondre soit à un agent réducteur comme le dithiothréitol (DTT) dans une solution, soit à l'exposition à la lumière UV, tout en ayant le nombre minimum des groups stimuli-réactifs dans la structure du copolymère (deux unités par chaîne). Nos investigations ont révélé que les micelles de ce copolymère tribloc peuvent être perturbées de différentes façons. Lorsqu'un seul stimulus est appliqué, l'enlèvement d'un type des chaînes de polymère hydrophile à partir de la couronne de micelles, soit le PEO par clivage par oxydo-réduction ou le PDMAEMA par photoclivage, entraîne un effet limité de déstabilisation sur la dispersion des micelles. L'agglomération de quelques micelles apparaît mais la dispersion reste essentiellement stable. En revanche, en cas d'utilisation combinée des deux stimuli qui clivent à la fois le PEO et le PDMAEMA, une agrégation importante du polymère se produit à la suite de l'élimination de l'amphiphilicité du polymère. // Abstract : Stimuli-responsive block copolymers (SR-BCPs) and their assemblies, such as micelles, vesicles and hydrogels, can undergo physical or chemical changes in response to changing environmental conditions. For an excellent SR-BCP, usually, slight changes in the environment are sufficient to induce relatively drastic changes in either the conformation or structure or properties of the polymer. Stimuli-reactive polymers are often referred to as smart polymers and they have great application potential in many fields. Over the past two decades, particular research and development interest has been focused on exploiting SR-BCP assemblies as drug delivery systems (DDSs). In many cases, stimuli-induced changes in the structure or morphology of BCP assemblies (drug carriers) can result in the release of loaded species, sometimes in a spatially and temporally controllable manner by choosing an appropriate stimulus and adjusting the parameters of the used stimulating method. Generally speaking, by having a certain type of stimuli-reactive moieties in the structure, SR-BCP assemblies have an ability to recognize a specific stimulus and react to its presence accordingly. Despite the tremendous progress achieved on SR-BCPs, a number of fundamental issues remain to be addressed in order to enable real-life applications of these smart polymers. Of them, an increasing level and complexity of control on SR-BCPs as well as the sensitivity with which these polymers react to stimuli are key and challenging. It is highly desirable to obtain a fast reaction under the action of a modest stimulation. To this end, fundamental research is necessary on rational and creative BCP structural design as well as on development of stimulation methods that can amplify the effect of a stimulus. The research work presented in this thesis falls into this important topic. More specifically, we studied BCP micelles that are responsive to two types of stimuli. On the one hand, we investigated an amplification mechanism based on coupling the ultrasound reactivity with the thermosensitivity of BCPs. On the other hand, we developed a BCP structural design that allows micelles to be disrupted by either light or redox agents while having the minimum number of stimuli-reactive moieties in the polymer structure. Our research provided new insights into and suggested new means on how the issues of sensitivity and complex control of SR-BCP micelles can be tackled, thus contributing to the advancement of fundamental knowledge. The core of this thesis is comprised of three publications resulting from the projects realized in our research work. In order to couple the ultrasound sensitivity and thermosensitivity, in the first project, we carried out studies to find possible polymer structures that are susceptible to be affected by ultrasound. We conducted a comparative study on the disruption of the micelles formed by various BCPs and the concomitant release of an encapsulated hydrophobic dye (Nile Red) by high-intensity focused ultrasound (HIFU). It was found that all micelles formed by the four synthesized diblock copolymers, being composed of a hydrophilic poly(ethylene oxide) (PEO) block and a different polymethacrylate hydrophobic block, could be disrupted by ultrasound. However, the extent of the micellar disruption and dye release was found to be influenced by the chemical structure of the micelle-core-forming hydrophobic polymethacrylate. In particular, micelles of PEO-b-PIBMA (poly(1-(isobutoxy)ethyl methacrylate)) and PEO-b-PTHPMA (poly(2-tetrahydropyranyl methacrylate)), whose hydrophobic blocks have a labile acetal unit in the side group and are more likely to undergo ester hydrolysis, could be disrupted more severely by ultrasound, giving rise to a faster release of Nile Red. By contrast, micelles of PEO-b-PMMA (poly(methyl methacrylate)), whose polymethacrylate block is more stable, appear to be more resistant to ultrasound irradiation and exhibit a slower rate of dye release than other BCPs. Moreover, infrared spectra recorded with micelles before and after ultrasound irradiation of the aqueous solution of the micelles give evidence for the occurrence of chemical reactions, most likely hydrolysis, for PEO-b-PIBMA and PEO-b-PTHPMA, but absence of chemical reactions for PEO-b-PMMA. The effect of BCP chemical structure on the reaction of micelles to high-frequency HIFU irradiation shows the perspective of designing and developing ultrasound-sensitive BCP micelles for ultrasound-based delivery applications. On the basis of the first project, in the second project, we demonstrated a new approach that could amplify the effect of HIFU on the disassembly of BCP micelles in aqueous solution. By introducing a small amount of ultrasound-labile comonomer units into the micelle core-forming thermosensitive polymer, the ultrasound-induced reaction of the comonomer could increase the lower critical solution temperature (LCST) of the thermosensitive polymer due to a polarity change, which renders the BCP soluble in water without changing the solution temperature and, consequently, results in disassembly of BCP micelles. To prove the validity of this new mechanism, we synthesized and investigated a diblock copolymer of PEO-b-P(MEO[subscript 2]MA-co-THPMA) (MEO[subscript 2]MA stands for 2-(2-methoxyethoxy)ethyl methacrylate). In the thermosensitive random copolymer block P(MEO[subscript 2]MA-co-THPMA), which is hydrophobic at T>LCST, THPMA was chosen due to its greater reactivity under HIFU than other monomer structures investigated in the first project. We found that HIFU could indeed increase the LCST of the P(MEO[subscript 2]MA-co-THPMA) block and, as a result, dissociate the BCP micelles at a constant temperature. A [superscript 13]C NMR spectral analysis provided critical evidence that hydrolysis of the THPMA groups occurs under HIFU irradiation and the micellar disassembly originates from an increase in the LCST due to the ultrasound-induced conversion of hydrophobic comonomer units of THPMA onto hydrophilic methacrylic acid (MAA). This ultrasound-changeable-LCST approach is general and can be applied by exploring other ultrasound-labile moieties in the BCP design. By transducing an ultrasound-induced effect into a changing thermosensitivity of the micelle core-forming block, this study demonstrated a new amplification and control mechanism for SR-BCP micelles. The third project presented in this thesis dealt with a rational BCP design that had a specific purpose: allowing BCP micelles to be disrupted by two types of stimuli while using the minimum number of stimuli-reactive moieties in the BCP structure. The unveiling of such BCP structures provides insight into how to make BCP micelles sensitive to stimuli. To do this, we designed and synthesized a new amphiphilic ABC-type triblock copolymer, namely, poly(ethylene oxide)-disulfide-polystyrene- o-nitrobenzyl-poly(2-(dimethylamino)ethylmethacrylate) (PEO-S-S-PS-ONB-PDMAEMA), which features a redox-cleavable disulfide linkage between the PEO and PS blocks as well as a photocleavable ONB group as the junction of the PS and PDMAEMA blocks. We demonstrated that this design is a useful strategy to allow BCP micelles to respond to both a reducing agent like dithiothreitol (DTT) in solution and exposure to UV light while having the minimum number of stimuli-reactive moieties in the block copolymer structure (two units per chain). Our investigations found that the micelles of this triblock copolymer could be disrupted in different ways. When only one stimulus is applied, the removal of one type of hydrophilic polymer chains from the micelle corona, either PEO by redox-cleavage or PDMAEMA by photocleavage, results in a limited destabilization effect on the dispersion of the micelles. The agglomeration between a few micelles appears but the dispersion remains essentially stable. By contrast, under combined use of the two stimuli that cleaves both PEO and PDMAEMA, severe polymer aggregation occurs as a result of elimination of the polymer amphiphilicity. Moreover, by loading the hydrophobic Nile Red in the micelles, the fluorescence quenching of the dye by aqueous medium under the different uses of the two stimuli appears to correlate with the different extents of the micellar disruption. // 摘要 : 刺激响应嵌段共聚物（SR-BCPs）和它们的自组装体（例如胶束、囊泡和水凝胶）可以对环境的改变做出物理或者化学变化的响应。对于优良的SR-BCP，在通常情况下，环境中的微小变化都足以诱导无论是在聚合物构象或者结构或者性能上相对很大的变化。刺激-反应性聚合物通常被称为智能聚合物，它们在许多领域具有很大的应用潜力。在过去的二十年中，专业的研究和新产品的开发一直聚焦在利用SR-BCP自组装体作为载药体系（DDSs）。在许多情况下，刺激诱导BCP自组装体（药物载体）结构或者形貌的改变都可以导致加载药物的释放。通过选择适当的刺激和调节用于刺激方法的参数，可以实现加载药物在空间和时间上的可控释放。一般来说，通过具有特定类型的刺激-反应性结构部分，SR-BCP自组装体就具有了识别特定刺激并做出相应反应的能力。 尽管SR-BCPs已经取得了巨大的发展，但是使这些智能聚合物能够在现实生活中得到应用，一些根本性的问题仍然需要加以解决。其中的关键和挑战是增加对SR-BCPs控制的深度和复杂性，以及对刺激响应的敏感度。使SR-BCPs能够在适度的刺激作用下做出快速的反应是人们梦寐以求的。为此，对于合理地创造性地设计BCP结构以及发展可以放大刺激效应的刺激方法的基础研究是非常有必要的。在本论文中提出的研究工作属于这一重要课题。具体来说，我们研究了双重刺激响应BCP胶束。一方面，基于BCPs的超声温度双重敏感性，我们研究了一种放大机制。另一方面，我们开发设计了一种在聚合物结构中只含有最少数目刺激-反应单元的BCP结构，可以让胶束被光或者还原剂破坏。我们的研究对于如何解决SR-BCP胶束的敏感性和复杂可控性提出了新的见解和方法，从而有利于基础知识的进步。 本论文的核心是由三篇已经发表的研究工作组成。为了实现超声和温度双重敏感性，在第一个研究课题中，我们对于容易受超声影响的聚合物结构进行了研究。我们比较了由不同BCPs组成的胶束结构在高强度聚焦超声（HIFU）作用下的破坏情况以及伴随着的包覆疏水染料（尼罗红）的释放情况。实验结果显示，四种以聚环氧乙烷为亲水端，不同的聚甲基丙烯酸酯为疏水端的两嵌段聚合物胶束都可以被超声扰动。然而，形成胶束疏水内核的聚甲基丙烯酸酯的化学结构影响胶束破坏和染料释放的程度。特别是，PEO-b-PIBMA（聚（ 1-（异丁氧基）乙基甲基丙烯酸酯） ）和PEO-b-PTHPMA（聚（2-四氢吡喃基甲基丙烯酸酯） ）的疏水端具有不稳定的酯键侧基，因此在超声作用下更容易酯键水解。他们的胶束也更容易 被超声扰动，从而更快的释放尼罗红。相比之下，PEO-b-PMMA（聚甲基丙烯酸甲酯）的聚甲基丙烯酸酯链段比较稳定。因此相对于其他胶束，PEO-b-PMMA胶束在超声下更稳定，释放染料的速度也相对较慢。根据超声辐照前后胶束水溶液的红外光谱显示，PEO-b-PIBMA和PEO-b-PTHPMA在超声辐照下发生了水解反应，但是PEO-b-PMMA没有发生化学反应。在高频率HIFU辐照下，BCP的化学结构对胶束反应的影响展现了设计和发展应用超声-敏感BCP胶束的新视角。 在第一个研究课题的基础上，在第二个研究课题中，我们展示了一种可以放大HIFU在水溶液中对BCP胶束破坏效果的新方法。通过在形成胶束内核的温敏性聚合物中引入少量的超声不稳定共聚单体，由于超声诱导共聚体极性的变化从而增加温敏性聚合物的最低临界溶液温度（LCST）。这使得在没有改变溶液温度的情况下，BCP溶于水，并进一步导致BCP胶束的瓦解。为了证明这种新机制的可行性，我们合成并研究了二嵌段共聚物PEO-b-P(MEO2MA-co-THPMA) （MEO2MA 代表2-（2-甲氧基乙氧基）乙基甲基丙烯酸酯）。当T > LCST时，无规的热敏嵌段共聚物P(MEO2MA-co-THPMA)是疏水的。选择THPMA是因为在第一个研究课题里，相比于其他结构的单体，它对于HIFU的辐照更敏感，具有更大的反应活性。我们发现， 通过HIFU的辐照确实可以增加P(MEO2MA-co-THPMA)链段的LCST，导致BCP胶束在温度不变的情况下瓦解。13C NMR 提供了关于超声诱导THPMA基团水解和由于超声诱导使疏水的THPMA共聚单元转变成亲水的MAA从而使LCST增加进一步导致胶束瓦解的关键证据。这种超声改变LCST的方法具有普遍意义，可以被用来探索在BCP设计中其他的超声不稳定基团。通过把超声诱导效应转换成胶束内核的温敏性变化，这项研究展示了一种全新的SR-BCP胶束的放大和控制机制。 在这篇论文中所展示的第三个研究课题是设计一个具有特定目的的合理的BCP结构。即允许在使用最少的刺激响应官能团的情况下，BCP胶束可以在两种刺激下瓦解。这种BCP结构的展示可以使我们更深入的了解如何使BCP胶束对刺激敏感。为此，我们设计并合成了新的两亲性ABC型三嵌段共聚物，即聚（环氧乙烷） - 二硫化物 - 聚苯乙烯 - 邻 - 硝基苄基 - 聚（ 2 - （二甲基氨基）乙基甲基丙烯酸酯） (PEO-S-S-PS-ONB-PDMAEMA)。它在PEO和PS嵌段之间具有可还原裂解的二硫键，在PS和PDMAEMA嵌段之间具有可光裂解的ONB基团。我们证实，对于使具有最少数量的刺激-反应官能团（每条分子链上仅有两个）的BCP胶束可以同时在还原剂二硫苏糖醇 （DDT）水溶液中和紫外光照下发生响应，此设计是一种行之有效的策略。我们研究发现，这种三嵌段共聚物胶束可以以不同的方式被破坏。当只施加一种刺激时，无论是还原裂解PEO链段，或是光裂解PDMAEMA链段，都只有一种亲水链从胶束外壳被移走，这都只能导致胶束分散有限的不稳定。虽然一些胶束之间发生了团聚，但是分散体系总体上基本保持稳定。与之相对的，在两种刺激同时作用的情况下，PEO和PDMAEMA链段的同时断裂使聚合物的两亲性消失，从而导致聚合物严重的聚集。此外， 在两种刺激不同的施加情况下，通过在胶束中装载疏水尼罗红的方式，结果显示染料的荧光在水中的淬灭与胶束被破坏的不同程度有关。

Realisation d'un dispositif experimental permettant de mesurer les variations de la lumiere diffusee, apres saut de temperature, dans un domaine de temps compris entre 10 mu s et 100 ms. Application aux etudes cinetiques de solutions micellaires

碩士
國立臺灣大學
化學工程學研究所
106
As an alternative for high energy-intensive reverse osmosis (RO) in seawater desalination, the novel approach known as forward osmosis (FO) has recently attracted much attention. Unlike RO which uses the high pressure difference as the driving force, FO utilizes the chemical potential gradient, or osmotic pressure, to drive the mass transfer. However, some studies showed that FO is actually not an energy-efficient approach, which may require more thermal energy and lead to higher cost in total. A new desalination scheme using lower critical solution temperature (LCST) ionic liquids as the draw solutes is presented. Despite higher energy consumption, the approach could replace the high cost electricity with low cost waste heat in plants or solar heat in the overall process. The osmotic pressure, required work, LCST and the miscibility gap are the most significant factors for the evaluation of the feasibility of ionic liquid draw solutes. In this work, we use COSMO-SAC 2010 + Pitzer-Debye–Hückel (PDH) model to perform a priori and efficient prediction of phase behavior. In the model the molecular structures are the only input in the model. We show that COSMO-SAC is able to differentiate the LCST and upper critical solution temperature (UCST) mixtures. Though our model provides poor quantitative prediction of LCSTs and the miscibility gaps (ARD%-LCST = 40.00%; ARD%-LLE 35.22%), the model appears to have great performance in qualitative agreement with experimental data. The thermodynamic properties including osmotic pressure, enthalpy of mixing, and the theoretical minimum work for the process are also evaluated. We analyze the temperature effect near the spinodal boundaries in order to have a molecular insight into LCST-positive phase behavior. Our results show that it is the preference of high entropy at high temperature that dominate in LCST-negative phase separations, while competition between molecular interactions, especially the hydrogen bonding interactions, play a more important role in the temperature dependence in the LCST-type phase separation. It is also demonstrated by our model that though with much higher required thermal energy, hybrid FO + RO process consume less electrical duty theoretically, allowing an energy-efficient use of waste heat. We propose a quick and feasible procedure for the screening ionic liquid draw solutes for FO processes.

碩士
長庚大學
化工與材料工程研究所
95
The objective of this research was to adjust the lower critical solution temperature (LCST) of poly (N-isopropylacrylamide)(PNIPAAm) copolymer hydrogel containing different amounts of acrylic acid (AAc) through free-radical polymerization. The resulting NIPAAm-co-AAc copolymers were grafted to a isopore polycarbonate membrane to prepare composite membranes. DSC analysis was used to illustrate the LCST changes for hydrogel. The water swelling ratio at various temperatures and pH values were determined to confirm the thermo- and pH- responses of the hydrogels. The grafting yield and membrane thickness increased with AAc content in composites. The characteristic functional groups of AAc were observed using FTIR. The swelling ratio increased and the contact angle decreased with AAc due to its hydrophilic nature. The water permeability and drug 4-acetamidophenol release permeability increased as a function of temperature. All the experiments showed that the LCST was increased with AAc contect. The hydrogel consisting of 1.7 gram and 0.02 microliter AAc showed an LCST around 37℃. Furthermore, the permeability on-off ratio of the composites was higher at higher AAc concentration. In conclusion, the composite membranes offer potential for drug controlled applications.

Thermoresponsive polymers such as poly(N-isopropylacrylamide) (PNIPAM) have lower critical solution temperature (LCST) in aqueous solutions. Below the LCST, these polymers are hydrophilic with an extended coil conformation. Above the LCST, they undergo a sharp phase transition to form a collapsed hydrophobic conformation. The LCSTs are also affected by cosolutes and the effects of anions on LCSTs follow the Hofmeister series. We successfully used a simple digital melting point apparatus to study the effects of heating rates, solvent compositions, cosolutes, and redox state, on the LCSTs of thermoresponsive polymers. Moreover, the temperature range of the apparatus allowed for analyses at much higher temperatures and provides a simple way to examine irregular clouding behavior in more complex systems. Meanwhile, stimuli-responsive surfaces grafted with thermoresponsive polymers can switch from hydrophilic to hydrophobic thermally. As the LCST can be subsequently changed with the addition of salts, the salt effects on the wettability of these thermoresponsive surfaces will dramatically impact the surface performance. In this dissertation, I prepared PNIPAM/SiO2 nanocomposite surfaces by a covalent layer-by- layer assembly procedure and such surfaces were then used in studies of salts effects on surface wettability. Both the effects of anions and cations on the changes of advancing angles (Delta Theta a) of the PNIPAM/SiO2 nanocomposite surfaces were significant (Delta Theta a up to 90 degrees). The anion effects on the surface wettability followed the Hofmeister effect as expected. Parallel studies on solution showed that variation of cations had a large effect on the LCST of PNIPAM too. Moreover, analyses of the Theta a and LCST data using activity instead of using concentration showed different orders for the cation effects which were readily grouped by the cation charge numbers. No difference was seen for the anion effects in similar studies. AFM studies showed that surface morphology changes were correlated with the Delta Theta a.

Yes
Highly-branched poly(N-isopropyl acrylamide)s in water pass through coil-to-globule transitions. Using calorimetry and the colour change of a solvatochromic dye within the polymer, we show that some compositions have biphasic core–shell morphologies, with globular cores and open coil shells. The two-phase structure is favoured by increased branching and arises because the chain ends penetrate only to a limited degree into the polymer coil.

abstract: Minimally invasive endovascular embolization procedures decrease surgery time, speed up recovery, and provide the possibility for more comprehensive treatment of aneurysms, arteriovenous malformations (AVMs), and hypervascular tumors. Liquid embolic agents (LEAs) are preferred over mechanical embolic agents, such as coils, because they achieve homogeneous filling of aneurysms and more complex angioarchitectures. The gold standard of commercially available LEAs is dissolved in dimethyl sulfoxide (DMSO), which has been associated with vasospasm and angiotoxicity. The aim of this study was to investigate amino acid substitution in an enzyme-degradable side group of an N-isopropylacrylamide (NIPAAm) copolymer for the development of a LEA that would be delivered in water and degrade at the rate that tissue is regenerated. NIPAAm copolymers have a lower critical solution temperature (LCST) due to their amphiphilic nature. This property enables them to be delivered as liquids through a microcatheter below their LCST and to solidify in situ above the LCST, which would result in the successful selective occlusion of blood vessels. Therefore, in this work, a series of poly(NIPAAm-co-peptide) copolymers with hydrophobic side groups containing the Ala-Pro-Gly-Leu collagenase substrate peptide sequence were synthesized as in situ forming, injectable copolymers.. The Gly-Leu peptide bond in these polypeptides is cleaved by collagenase, converting the side group into the more hydrophilic Gly-Ala-Pro-Gly-COOH (GAPG-COOH), thus increasing the LCST of the hydrogel after enzyme degradation. Enzyme degradation property and moderate mechanical stability convinces the use of these copolymers as liquid embolic agents.
Dissertation/Thesis
Masters Thesis Biomedical Engineering 2019

碩士
國立臺灣科技大學
化學工程系
105
PNIPAm is a temperature-responsive polymer that undergoes a reversible lower critical solution temperature (LCST) phase transition from a swollen hydrated state to shrunken solid state. This work studied the effects of different initiators on the molecular weight and LCST of Poly(N-isopropylacrylamide) (PNIPAm). The common initiator azobisisobutyronitrile (AIBN) and sodium persulfate (SPS) which used in other polymerization systems were empolyed here. In addition , barbituric acid (BTA) also can initiate free radical polymerization with the reactive groups one >CH2 and two >NH groups in its structure. Thus, the polymerization and characterization of N-isopropylacrylamide (NIPAm) with novel initiator BTA was investigated. We also copolymerized hydrophilic and hydrophobic monomer with NIPAm respectively for adjusting the LCST behavior of PNIPAm, and find that both 2-hydroxyethyl acrylate (2-HEA) and 2-ethylhexyl acrylate (2-EHA) can decrease the LCST of PNIPAm. The LCST behavior of the aqueous solutions of polymers and copolymers was measured by differential scanning calorimetry (DSC). The technique of NMR, GPC and EPR were employed to study the reactivity of BTA. Further, non-isothermal LCST phase transition kinetics of PNIPAm was investigated by the DSC technique. The advanced isoconversional method (model-free method) can be used to determine the effective activation energy of non-isothermal sol-gel behavior of PNIPAm. The sol-gel transition process of increasing temperature involved forming PNIPAm nucleation and particle growth, and then particle shrink and aggregate simultaneously；on the other hand, the sol-gel transition of cooling PNIPAm related to form the hydrogen-bonding between H2O and PNIPAm and particle swelling and dissolution in H2O. The detail of the phase transition mechanism will show in this study .

Biophysics has seen unprecedented progress, applying concepts from physics to study intriguing biological phenomena. Further advances in this field require fundamental understanding of various processes at the nanoscale and development of appropriate methods and models for different applications. Molecular simulation is playing an ever-increasing role for these purposes. In this thesis, I have examined the structure, dynamics and thermodynamics of various biomolecules of interest using molecular simulation and theoretical modeling. The thesis is organized as follows. In the 1st chapter, I briefly introduce various bioactive molecules and relevant biological phenomena. The 2nd chapter consists of detailed descriptions of simulation methodologies and theoretical frameworks. These include classical molecular dynamics (MD) simulations, advanced sampling techniques for free energy calculations, and various entropy calculation methods. In chapter 3, we propose a carbon nanotube (CNT)-based drug-delivery method. One of the major challenges of nanomedicine and gene therapy is the effective delivery of drugs and genes across cell membranes. Generally, bioactive molecules used as drugs or drug-delivery vehicles cannot passively pass through the cell membrane due to the high penalty associated with membrane rupture. We show via MD simulations that molecules of various shapes, sizes and chemistries can spontaneously enter a membrane-spanning CNT nanopore. We study the thermodynamics of entry of several molecules of interest, such as dendrimers, asiRNA, ssDNA and ubiquitin protein. We show that another free CNT can spontaneously enter the CNT nanopore and eject the encapsulated molecule out of the nanopore. In this way, a macromolecule can be translocated across the cell membrane. We also verify the thermodynamic feasibility of the proposed method. This method should work for other molecules as well, and hence could be potentially useful for drug-delivery applications. The fourth chapter deals with the understanding of complex force-dependent protein unfolding kinetics. For some proteins, e.g., ubiquitin, the unfolding rate at very low forces doesn't vary much up to a critical force, after which the rate increases exponentially by increasing the force further. This crossover in the unfolding rate can be due to one of the following two scenarios. First, there are two unfolding pathways for the protein and pathway-switch occurs after the critical force. Second, the unfolding pathway can change continuously due to force-dependent modifications in the free-energy landscape. By performing nonequilibrium MD simulations of ubiquitin at forces ranging 20–800 pN, we find a crossover in the unfolding rate and show that the crossover is due to the second scenario. We rationalize the results by using multidimensional transition state theory. The findings from this chapter will have implications in understanding the folding/unfolding kinetics of protein which is one of the outstanding problems of the current century. In the 5th chapter, we decipher the molecular mechanism and thermodynamic driving force for lower critical solution temperature (LCST) phase behavior of the aqueous solution of proteins induced by multivalent ions, observed recently in experiments. LCST phase behavior manifests itself as phase separation of the protein–salt solution upon heating. This has been attributed to entropy effects. We use MD simulation along with the two-phase thermodynamic method for entropy calculation. Our simulations reveal two key steps that help in explaining the LCST phase behavior. First, the cations binding to the protein: this requires the release of tightly bound water molecules from the solvation shells of cations and partial desolvation of the protein surface residues, which are indeed entropy driven. Second, the protein-bound cations attract other proteins present in the solution, whose binding is again entropy driven, resulting in LCST behavior. By performing series of simulations of protein in chloride solutions of various cations (Na+, Ca2+, Mg2+ and Y3+), at temperatures ranging 283–323 K, we suggest that multivalent cation binding to any negatively charged surface can be entropy driven. These findings have direct implications for tuning the phase behavior of soft matter systems, such as reentrant condensation and protein crystallization. In a broader context, molecular-level understanding of interactions of heavy metals—usually not found in healthy cells—with different biomolecules can provide insights for carcinogenicity and neurotoxicity induced by exposure to such environmental contaminants. In chapter 6, we provide a molecular-level understanding of how intercalation of a drug affects DNA mechanics. Most of the anticancer drugs are known to intercalate in-between two consecutive base-pairs of a double-stranded DNA (dsDNA). These DNA-intercalators are believed to hinder DNA replication and transcription, eventually leading to cell death—thus acting as anticancer drugs. We probe, using MD simulations, change in the mechanical properties of the intercalated drug–DNA complexes for two intercalators, daunomycin and ethidium. We find that, upon drug intercalation, the persistence length and bending modulus of dsDNA don’t change significantly, whereas its stretch modulus increases by as much as 65%. Steered MD simulations also reveal that it requires higher forces to stretch the drug-intercalated dsDNA complexes than the bare dsDNA. Adopting various pulling protocols to study force-induced DNA melting, we find that dissociation of the dsDNA complex becomes difficult in the presence of intercalators. The results obtained here provide a plausible mechanism of action of the anticancer drugs—i.e., via modifying the mechanical properties of DNA. Finally, in chapter 7, I summarize all the results with concluding remarks and future outlooks

Smart windows that modulate solar radiation by changing their optical state in response to temperature stimulus are developing as promising solutions towards reducing the energy consumption of buildings. The market adoption of such systems has been slow due to the barriers in scalability, cost, as well as complexity in their integration into existing systems. Aiming these features, we have proposed a retrofit smart window design based on the temperature-responsive polymer Methyl Cellulose (MC). The system utilizes a sustainable, earth abundant and cost-effective cellulose based thermo-responsive material to transform existing windows to a thermally dynamic smart window system. The observed optical change of MC from transparent to opaque state is dependent on temperature and is triggered by the thermodynamic mechanism of reversible coil-globule transition, which results in a stable performance of the proposed device. Its solar modulation ability was studied using ultraviolet-visible- spectroscopy. Effect of MC concentration and various salts on the optical performance were investigated. It was found that the transition temperature the polymer can be tuned by varying MC concentration and by adding salts to the system. The tunability of transition temperature is a function of the concentration of salt and the type of anion in the salt. It was observed that the transition temperature of the window can be tuned between to , allowing a wide range of control over switching temperature. Controllable LCST, low freezing point, sustainable base material, scalable production, low cost, retrofit system makes them ideal candidates for smart window applications.

Several analytical mean field models are presented for the class of stimuli responsive polymers that are driven by the lower critical solution temperature (LCST) transition. For solutions above the polymer crossover concentration, a hybrid model combines lattice-fluid excluded volume and van-der-Waals interactions with a combinatorial approach for the statistics of hydrogen bonding, hydration, and ionic bonding. This approach yields models for the LCST of both neutral polymers and lightly charged polyelectrolytes in aqueous salt solution. The results are shown to be in semi-quantitative agreement with experimental data for the cloud point of polyethylene oxide (PEO) in aqueous solution with various salts, and some aspects of the lyotropic series are reproduced. Results for lightly charged polyelectrolytes are compared to and shown to be in qualitative agreement with aspects of experimentally observed behavior. Finally, a framework is established for extension of these models to further aspects of the lyotropic series and polyelectrolyte behavior. At the nanoscale, lattice fluid (LF) and scaled particle theory (SPT) approaches are employed to model the LCST-related coil-globule-transition (CGT) of isolated polymer chains in highly dilute solution. The predicted CGT behavior semi-quantitatively correlates with experimental results for several polymer-solvent systems and over a range of pressures. Both the LF and SPT models exhibit a heating induced coil-to-globule transition (HCGT) temperature that increases with pressure until it merges with a cooling induced coil-to-globule transition (CCGT). The point at which the CCGT and HCGT meet is a hypercritical point that also corresponds to a merging of the lower critical and upper critical solution temperatures. Theoretical results are discussed in terms of a generalized polymer/solvent phase diagram that possesses three hypercritical points. Within the lattice model, a dimensionless transition temperature [author gives mathematical symbol] is given for a long chain simply by the equation [author gives mathematical equation], where [part of the equation] is the bulk solvent occupied volume fraction at the transition temperature. Furthermore, there is a critical value of the ratio of polymer to solvent S-L characteristic temperature below which no HCGT transition is predicted for an infinite chain.
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Research Doctorate - Doctor of Philosophy (PhD)
Stimulus-responsive polymers are useful components of smart materials as their conformation can be switched reversibly by changing environmental conditions such as pH and temperature. End-grafting these polymers at a high areal density to form a polymer brush allows the switchable modification of surface properties such as adhesion and lubricity. These surface coatings have shown particular promise for biomedical applications such as controlled cell adhesion and drug delivery. In many of these applications the concentration of salt is significant. The concentration and, more importantly, the identity of salt present in solution affects a wide range of phenomena including bubble-bubble coalescence, protein stability and even the surface tension at the air-water interface. These specific ion effects have also been observed in stimulus-responsive polymer brushes, but are poorly understood on a theoretical level. Therefore a comprehensive experimental and theoretical understanding of these effects is required for informed design of smart polymer brushes. This thesis outlines advances in the understanding of the influence of ion identity and concentration on two major classes of responsive polymer brushes: pH responsive weak, polycationic brushes and neutral thermoresponsive polymer brushes. Experimental studies utilise thiocyanate and acetate as representative weakly and strongly hydrated anions respectively. The specific ion responses of the two classes show opposing behaviour, with polycationic brushes exhibiting a lower, and thermoresponsive polymers a higher degree of swelling in increasing concentrations of thiocyanate, for example. In this case, the difference arises from the neutralisation of charge by thiocyanate in the polycationic brushes, while binding of thiocyanate increases the surface charge of thermoresponsive polymers. The polymer hydrophilicity was found to have a significant impact on the magnitude of the specific ion response. Hydrophobic polycationic brushes showed a stronger response due to a greater preference for collapsed structures when neutralised while the specific ion response was greater for hydrophilic thermoresponsive polymers as the polar nature of their surfaces favours ion binding. Neutron reflectometry (NR) was utilised as a powerful technique for determining changes in the structure of the brushes perpendicular to the interface. The diffuse nature of the brush can lead to challenges when analysing reflectivity data from NR. However, development of new analytical techniques allows the volume fraction profile of the studied polymer brushes to be determined with confidence. This has been used to provide direct evidence of the theoretically predicted vertical phase separation of thermoresponsive poly(N-isopropylacrylamide). However, even greater insight is achieved when paired with other techniques. For example, complementary atomic force microscopy measurements show that the ions can affect the mechanical properties of a brush beyond their influence on its overall degree of swelling. Neutron reflectometry was also used to validate an extended numerical self-consistent field (nSCF) theory of polycationic brushes. This theory showed that addition of a single Flory-Huggins parameter related to the strength of hydration of the counterion was sufficient to account for the observed specific ion effects. Overall, this research represents a significant step forward to understanding specific ion effects on stimulus-responsive polymer brushes. These effects could not be directly accounted for by prior studies of equivalent ungrafted polymer in the literature. That is, the geometry of the system has been found to be a significant factor. This work also briefly introduces studies of polymer brushes in mixed salt solutions, as the vast majority of existing studies on all stimulus-responsive materials have been carried out in a single electrolyte. More detailed studies of the impact of mixed salts are required if the real-world performance of stimulus-responsive polymer brushes is to be predicted and understood.

The viscoelastic properties of a model binary polymer blend exhibiting an Upper Critical Solution Temperature (UCST) phase diagram were investigated by utilizing small amplitude oscillatory and steady shear measurements. A mixture of unentangled monodisperse poly(styrene) and poly (phenyl methyl siloxane) was used, and its phase diagram was established by turbidity and light scattering measurements. In the miscible region the concentration dependence of the viscosity was adequately described by a mixing rule accounting for the molecular surfaces. Near the phase separation temperature and far from the glass transition, critical concentration fluctuations dominated the linear viscoelastic response and were responsible for the observed thermorheological complexity. An appropriate quantitative account of these fluctuations resulted in the accurate rheological determination of both the binodal and spinodal temperatures, extending thus the applicability of relevant procedure originally developed for blends exhibiting lower critical solution temperature (LCST) behavior. In the phase separated regime, the elasticity of the dispersed phase undergoing spinodal decomposition was due to the interfacial tension, and the resulting normal stresses followed the scaling recently predicted by Onuki for molecular mixtures with large viscosity difference.

Thermo-responsive homopolymer poly(N-isopropylacrylamide), is a widely studied and used polymer. Our recent observations on thermal behavior of aqueous solutions of this polymer requires a short overview of existing results in order to understand the formation of different phases, both stable and unstable with the addition of hydrophilic Ionic liquids (ILs) 1-Butyl-3-methylimidazolium tetrafluoroborate ([BMIM][BF4]), 1-Butyl-3-methylimidazolium acetate ([BMIM][OAc]) and 1-Butyl-3-methylimidazolium thiocyanate ([BMIM][SCN]) to the system. PNIPAM is soluble in cold water due to its inter- and intramolecular hydrogen bonding but phase separates upon heating at T > 32 , which is its lower critical solution temperature (LCST). PNIPAM exists in an expanded coil like conformation in water below its LCST which gives a transparent homogenous solution but at T > LCST it undergoes hydrophobic collapse marked by cloudiness of solution and conformational change from coil to globule state. All aqueous PNIPAM solutions undergo phase separation or cloud point transition at T > 32 , regardless of the molar mass of the polymer. Room temperature Ionic liquids (ILs) are unique designer fluids because of the novel physico-chemical properties arising from their structure, which have tremendous implications in the field of IL as solvents or co-solvents for polymeric solutes. During recent years a number of different imidazolium based ILs have also been tested for solubilization and stabilization of proteins as well as polymers due to hydrogen bond formation of the IL ions. Recent studies have shown that certain imidazolium based ILs can decrease the LCST of PNIPAM aqueous solution by hydrophobic collapse/aggregation of the PNIPAM chains, as well as some can induce an upper critical solution temperature (UCST) behavior of PNIPAM in neat IL solution. Even so, experimental studies of such phase transition/ instability of thermoresponsive polymer-IL systems has been a challenging task. In this research we have explored the critical solution temperature (CST) type phase behavior of multicomponent systems i.e. PNIPAM in solution media of water, neat IL and aqueous solutions of IL. The overall fundamental challenge is to understand how the interactions among the components control both structure and dynamics of PNIPAM network in solution. For example the disruption of hydrogen bonding or desolvation interactions between blocks of a PNIPAM molecule and solvent molecules in aqueous mixtures that lead to a LCST type transition at higher temperatures. Interestingly, it was found in our case that PNIPAM shows both LCST and UCST-type phase transition in some aqueous solutions of hydrophilic IL [BMIM][BF4]. It was found for the first time that this IL can influence the LCST type behavior of PNIPAM in aqueous solutions based on our visual and experimental cloud point (CP) observations. In our experiments the effect of the ILs [BMIM][BF4] and [BMIM][OAc] is qualitatively similar to influence of Kosmotropic salts on the LCST of aqueous PNIPAM solutions as predicted by the Hofmeister series.

In dieser Arbeit wurde am Modell der Hydridbildung in Wasserstoff-beladenen, 5 nm bis 2000 nm dünnen Palladium-Schichten der Einfluß der Schichtdicke sowie mikrostruktureller und elastischer Zwangsbedingungen auf die Thermodynamik von Phasenübergängen 1. Ordnung untersucht. Grundlage der Untersuchungen ist eine H-induzierte Volumendehnung des Palladiums, die infolge eines Konzentrationshubs ∆c_H bei der Hydridbildung sprunghaft erfolgt. Aus der Volumendehnung resultieren an der Schicht-Substrat-Grenzfläche und an inneren Grenzflächen wie Phasen- und Korngrenzen hohe mechanische Spannungsgradienten, die additiv zum chemischen Potential μ_H des Wasserstoffs beitragen und die Stabilität der Hydridphase verändern. Der Einfluß mechanischer Spannungen auf das chemische Potential wird durch die Mikrostruktur der Schichten modifiziert, die unterschiedliche H-Einlagerungsplätze im Palladium-Gitter mit einem Spektrum unterschiedlicher Platzenergien bereitstellt und die Kanäle eines möglichen Spannungsabbaus durch plastische Deformation der Schichten bestimmt. Ziel dieser Arbeit war es, die sich überlagernden Einflüsse der Mikrostruktur und mechanischer Spannungen auf die Thermodynamik der Hydridbildung experimentell zu separieren und aus ihnen resultierende Abweichungen von der Thermodynamik des massiven Pd-H-Systems unter Bezugnahme auf thermodynamische Modellvorstellungen zu quantifizieren. Durch gezielte Wahl der Herstellungsbedingungen präparierte Pd-Schichten texturiert nanokristalliner, multi-orientiert polykristalliner und epitaktischer Mikrostruktur wurden schrittweise mit Wasserstoff beladen. H-induzierte Änderungen des Spannungszustands, die Hydridbildung und plastische Änderungen der Schichten wurden in-situ insbesondere mit Methoden der Röntgendiffraktometrie, durch die Messung der Substratverbiegung, des elektrischen Widerstandes, der akustischen Emission der Schichten sowie mittels STM und Proton-Proton-Streuung untersucht. Hinsichtlich mikrostruktureller Änderungen der Schichten bei H-Beladung wurden Kaskaden kritischer Schichtdicken und Spannungszustände des Einsetzens plastischer Deformation gefunden. Bereits im Bereich der elastischen Schichtdehnung wurden diskrete Relaxations-Ereignisse beobachtet, die auf die Bewegung intrinsischer Defekte zurückgeführt wurden. Für Schichtdicken unterhalb von 22-34 nm wurde ein neuer Typ eines partiell kohärenten Phasenübergangs belegt, bei dem die Phasengrenzflächen während des gesamten Phasenübergangs kohärent verbleiben. Unter dem Einfluß der unterschiedlichen Mikrostrukturen und Spannungszustände der Schichten wurde eine signifikante Reduktion der elastischen H-H-Wechselwirkung – der Triebkraft der Hydridbildung – um 20-50 % gegenüber dem massiven System belegt. Für die Schichten beträgt E_HH 15-30 kJ/mol_H, während im massiven System E_HH = 36.8 kJ/mol_H. Der elastische Beitrag zur Reduktion der H-H-Wechselwirkung beträgt 2-5 kJ/mol_H. Er wächst für partiell kohärente Entmischung rasch an. Die entsprechenden Hydridbildungsenthalpien sind in Schichten um bis zu 3 kJ/mol_H erhöht. In lokal durch Faltenbildung relaxierten Schichten kann dies das räumliche Nebeneinander der α-Phase in haftenden Schichtbereichen und der Hydridphase in den Falten erzwingen. Darüber hinaus wurde gezeigt, daß die Druck-Konzentrations-Isothermen dünner Pd-H-Schichten im Bereich des Phasenübergangs unter dem Einfluß nicht-linearer mechanischer Spannungen eine stetige Steigung aufweisen können. Dies macht eine Modifikation der Grenzbedingung zur Bestimmung der kritischen Temperatur der Hydridbildung erforderlich, bei der die Steigung ∂μ_H/∂c_H | T=T_c explizit ausgewertet wird. Die resultierenden kritischen Temperaturen der Pd-H-Schichten sind bis zu 40 % gegenüber dem massiven System reduziert. T_c ist 340-490 K für die Schichten, während T_c = 563 K für das massive System. In allen Schichten wurde bei 300 K noch immer ein Phasenübergang gefunden. Insgesamt ließen sich die beobachteten Änderungen der Thermodynamik zumeist direkt an die Mikrostruktur und den Spannungszustand der Schichten koppeln, während allein an die Schichtdicke gebundene Finite-Size-Effekte bei den untersuchten Schichten von untergeordneter Bedeutung sind.