SYNTHESIS AND PROPERTIES OF BRANCHED SEMI-CRYSTALLINE THERMOSET RESINS Hans Claesson Royal Institute of Technology Fibre and Polymer Technology Stockholm 2003 Akademisk avhandling Som med tillstånd av Kungliga Tekniska Högskolan i Stockholm framlägges till offentlig granskning för avläggande av teknisk doktorsexamen fredagen den 5 september 2003, kl. 13.00 i kollegiesalen, administrationsbyggnaden, Valhallavägen 79, Kungliga Tekniska Högskolan, Stockholm. Avhandling försvaras på engelska. To my Wife Laura Abstract This thesis describes the synthesis and characterization of branched semi-crystalline polymers. Included in this work is the SEC characterization of a series of dendrimers. The branched semi-crystalline polymers were synthesized in order to investigate the concept of their use as powder coatings resins. This concept being that the use of branched semi-crystalline polymers in a UV-cured powder coating system may offer a lower temperature alternative thus allowing the use of heat sensitive substrates and the added benefit of a reduced viscosity compared to linear polymers. A series of branched poly(ε-caprolactone)’s (PCL) (degree of polymerization: 5-200) initiated from hydroxyl functional initiators were synthesized. The final architectures were controlled by the choice of initiator structure; specifically the dendritic initiators yielded starbranched PCL’s while the linear initiator yielded comb-branched PCL’s. The dendritic initiators utilized were: (1) a 3rd-generation Boltorn H-30, commercially available hyperbranched polyester with approximately 32 hydroxyl groups, (2) a 3rd-generation dendrimer with 24 hydroxyl groups, and (3) a 3rd-generation dendron with 8 hydroxyl groups. Linear PCL was synthesized for comparison. All dendritic initiators are based on 2,2bis(methylol) propionic acid. The comb-branched polymers were initiated from a modified peroxide functional polyacrylate. The resins were end-capped with methylmethacrylate in order to produce a cross-linkable system. The polymers and films were characterized using 1H NMR, 13C NMR, SEC, DMTA, DSC, FT-IR, FT-Raman, rheometry and a rheometer coupled to a UV-lamp to measure cure behavior. The star-branched PCL’s exhibited considerably lower viscosities than their linear counterparts with the same molecular weight for the molecular region investigated (2-550 kg mol-1). It was also found that the zero shear viscosity increased roughly exponentially with M. The PCL star-branched resins are semi-crystalline and their melting points (Tm) range from 34-50°C; films can be formed and cured below 80°C. The viscoelastic behaviour during the cure showed that the time to reach the gel point, a few seconds, increased linearly with molecular weight. The crossover of G’ and G’’ was used as the gel point. Measurement of mechanical properties of films showed that the low molecular weight polymers were amorphous while those with high molecular weight were crystalline after cure. The polymerization of 5,5-dimethyl-1,3-dioxane-2-one (NPC) from oligo- and multifunctional initiators was evaluated utilizing coordination and cationic polymerization. Two tin based catalysts, stannous(II) 2-ethylhexanoate and stannous(II) trifluoromethane sulfonate, were compared with fumaric acid. Fumaric acid under bulk conditions resulted in lower polydispersity and less chance of gelling. The synthesis of star-branched polymers was confirmed by SEC data. The star polymers exhibited a Tg at 20-30°C and a Tm at about 100°C. All semi-crystalline resins exhibited a fast decrease in viscosity at Tm. Blends of combbranched semi-crystalline resins and amorphous resins exhibited a transition behavior inbetween that of pure semi-crystalline resins and that of amorphous resins. The SEC characterization of a series of dendrimers with different cores and terminal groups showed that the core had an impact on the viscosimetric radius of the core while the terminal groups appeared to have no effect. Keywords: star-branched, semi-crystalline, comb-branched, ring-opening polymerization, poly(ε-caprolactone), dendritic, thermoset, low temperature curing, powder coating, UVcuring, poly(5,5-dimethyl-1,3-dioxane-2-one), size exclusion chromatography, rheology, dendritic aliphatic polyester I Sammanfattning Avhandlingen beskriver syntesen och karakteriseringen av en serie förgrenade delkristallina polymerer. Inkluderat i detta arbete är också SEC karakteriseringen av en serie av dendrimerer. De förgrenade delkristallina polymererna syntetiserades och karakteriserades för att undersöka ett koncept för deras användning som pulverbindemedel. Konceptet är att en delkristallin struktur tillsammans med UV-härdning kan resultera i en lägre härdtemperatur och på så vis möjliggöra användningen av pulverfärger på värmekänsliga substrat. En grenad struktur kan också ge en lägre viskositet. En serie av förgrenade poly(ε-kaprolakton)er (PKL) (polymerisationsgrad: 5-200) initierad från hydroxyfunktionella initiatorer syntetiserades. Den slutliga arkitekturen styrdes av valet av initiator. De dendritiska initiatorerna resulterade i stjärnförgrenad PKL och den linjära initiatorn resulterade i kamförgrenad PKL. De dendritiska initiatorerna som användes var: (1) en 3je-generations Boltorn H-30, kommersiellt tillgänglig hyperförgrenad polyester med cirka 32 hydroxylgrupper, (2) en 3je generations dendrimer med 24 hydroxylgrupper, (3) en 3rd-generations dendron med 8 hydroxylgrupper. Linjär PKL syntetiserades för jämförelse. Alla dendritiska initiatorer är baserade på 2,2-bis(metylol) propionat syra. Den kamförgrenade polymeren initierades från en modifierad epoxid funktionell polyakrylat. Polymererna funktionaliserades med metylmetakrylat för att ge en tvärbindningsbar polymer. Polymererna och filmerna karakteriserades med 1H NMR, 13C NMR, SEC, DMTA, DSC, FT-IR, FTRaman, reometer, och en reometer utrustad med en UV-lampa för att mäta härdbeteende. De stjärnförgrenade polymererna uppvisade en betydligt lägre viskositet än de linjära polymererna med samma molekylvikt (M) (i området 2-550 kg mol-1). Det observerades också att gräns skjuvviskositeten (η0) ökade exponentiellt med M, vilket var förväntat. PKL stjärnpolymererna är delkristallina och smältpunkten (Tm) är 34-50°C; filmer kan framställas och härdas under 80°C. Det viskoelastiska beteendet under härdning av de stjärnförgrenade polymererna visade att tiden till att nå gelpunkten, några sekunder, ökade linjärt med molekylvikten hos polymeren. G’=G’’ användes for att bestämda gelpunkten. Mätningen av de mekaniska egenskaperna hos härdade filmerna av de stjärnförgrenade polymererna visade att de filmer tillverkad från polymerer med låg molekylvikt var amorfa medan de med hög molekylvikt var delkristallina. Polymerisationen av 5,5-dimetyl-1,3-dioxan-2-one (NPK) från multifunktionella initiatorer utvärderades med koordinations- och katjonpolymerisation. Två tennbaserade katalysatorer och fumarsyra jämfördes. Fumarsyra in bulkreaktion resulterade i lägst polydispersitet och mindre risk för gelning jämfört med de tennbaserade katalysatorerna. Syntesen av stjärnförgrenade polymerer bekräftades av SEC-analys. Stjärnpolymererna hade ett Tg på 2030°C och ett Tm på ca. 100°C. Alla delkristallina polymerer uppvisade en snabb minskning av viskositeten vid Tm. Blandningar av delkristallina kampolymerer och amorfa polymerer uppvisade ett smält/mjuknings beteende mellan det av en ren delkristallin och amorf polymer. SEC karakteriseringen av en serie av dendrimerer med olika kärnmolekyler och terminala grupper visade att viskositetradien påverkades av kärnmolekylen men inte av de terminala grupperna. II List of Papers This thesis is a summary of the following papers: I “Synthesis and Characterisation of Star Branched Polyesters with Dendritic Cores and the Effect of Structural Variations on Zero Shear Rate Viscosity” H. Claesson, E. Malmström, M. Johansson & A. Hult Polymer (2002), 43(12), 3511-3518. II “Semi-Crystalline Thermoset Resins: Tailoring Rheological Properties in Melt using Comb Structures with Crystalline Grafts” H. Claesson, C. Scheurer, E. Malmström, M. Johansson, A. Hult, W. Paulus & R. Schwalm Submitted to: Progress in Organic Coatings. III “Star-Branched Poly(neopentyl carbonate)s” P. Löwenhielm, H. Claesson, E. Malmström & A. Hult Manuscript. IV “Rheological Behaviour during UV-curing of a Star-Branched Polyester” H. Claesson, M. Doyle, E. Malmström, M. Johansson, J-A. E. Månsson & A. Hult. Progress in Organic Coatings (2002), 44(1), 63-67. V “Synthesis and Characterization of Bis-MPA Dendrimers with Different Core and Terminal Groups” M. Malkoch, H. Claesson, P. Löwenhielm, E. Malmström & A. Hult Manuscript. III Table of Contents Abstract……………………………………………………………..…….. I Sammanfattning…………………………………………...……………… II List of Papers…………………………………………………………....…III 1. Purpose of the Study……………...………….………………………… 1 2. Background…………………………………..………………………… 2 2.1 Powder Coatings...……………………………………………..….……… 2 2.1.1 UV-Cured Powder Coatings……….………………………………. 4 2.2 Branched Polymers...………………………………...…………………… 6 2.2.1 Dendritic Polymers………………………………………………… 6 2.2.1.1 Dendrimers…….....…………………………………………... 6 2.2.1.2. Hyperbranched Polymers..……..……………………………. 8 2.2.2 Star-Branched Polymers…………….……………………………... 8 2.2.3 Comb-Branched Polymers…………………………………………. 9 2.3 Ring-Opening Polymerization………………………….………………… 9 2.3.1 Coordination Insertion Ring-Opening Polymerization……………..10 2.3.2 Cationic Ring-Opening Polymerization………………………….... 10 2.4 Rheology in the Molten State…………………………………………….. 10 2.4.1 Rheological Behavior of Linear Polymers………………………… 10 2.4.2 Rheological Behavior of Branched Polymers………………...…… 11 3. Syntheses and Chemical Characterization…………………………..…. 13 3.1 Monomers………………………………………………………………… 13 3.2 Star-Branched Poly(ε-caprolactone)’s……………………………………. 13 3.2.1 Synthesis…………………………………………………………… 14 3.2.2 NMR Characterization…………………………………………..…. 15 3.2.3 SEC Characterization……………………………………..……….. 16 3.3 Star-Branched Poly(neopentyl carbonate)’s………..……………....…….. 18 3.3.1 Synthesis………………………………………………………..….. 19 3.3.1.1 Monomer Synthesis………………………………………….. 19 3.3.1.2 Polymer Synthesis……………………………………………. 19 3.3.2 NMR Characterization………………………………………...…… 20 3.3.3 SEC Characterization…………………………………………..….. 22 3.3.4 Catalyst Evaluation………………………………………………… 23 3.3.5 Thermal Characterization…………………………………….……. 25 3.4 Comb-Branched Poly(ε-caprolactone)’s…………………………...…….. 26 3.4.1 Synthesis………………………………………………………….... 26 3.4.2 IR Characterization…………………………..…………………….. 27 3.4.3 SEC Characterization…………………………...…………………. 28 3.5 Bis-MPA Dendrimers…………………………………………………….. 29 3.5.1 SEC Characterization………………………...……………………. 30 4. Rheological Characterization………………………………………..…. 35 4.1 Zero Shear Viscosity of Star-Branched Poly(ε-caprolactone)’s…………. 35 4.2 UV-curing Rheological Behavior of Star-Branched Poly(ε-caprolactone). 36 4.3 Dynamic Viscosity from Solid to Molten State………………………..…. 42 4.3.1 Comb Poly(ε-caprolactone) and Blends…………….……………. 43 5. Film Characterization…………………………………………………... 45 5.1 Mechanical Properties of Star-Branched Poly(ε-caprolactone) Films…… 45 5.2 Comb Poly(ε-caprolactone) Films……………........................................... 46 5.2.1 Powder and Film Preparation……………………………………… 46 5.5.2 Film Properties……………………………………………….……. 47 6. Conclusions……………………………………………………….……. 49 7. Suggestions of Further Work………………………………...………… 51 Acknowledgements…………………………………….…………………. 52 References…………………………………………………….……….….. 54 Appendix A – Structures of the Different Star-Branched Polymers Appendix B – SECuc and Viscosity Data of all Star-Branched PCL’s Appendix C – Synthetic Scheme of Boltorn-PNPC 1. Purpose of the Study Thermoset resins are very important in industry were high demands are set on the final properties; applications such as adhesives, molding compounds and coatings. One area were thermoset resins have a significant share of the market in comparison to thermoplastic resins is in the area of powder coatings. Since the introduction of powder coatings, the industry has been striving to improve coating technology to widen its application to new markets such as wood coatings. UV-cured powder coating systems were recently introduced as an alternative to conventional thermal curing in an effort to capitalize on this new market. The goal of this body of work was to investigate a new powder coating concept, which would result in a reduction of the curing temperature. The approach was to investigate how changes in macromolecular architecture, molecular composition, molecular weight and introduction of crystallinity affect the properties relevant to powder coating applications, which include rheological, cure, and final film properties. In addition, the effects of molecular weight and architecture on resin crystallinity was also a subject of interest as was the relationship between resin structure and resin properties before, during and after curing. To obtain better overall knowledge of the relationship between architecture, functionality and properties in a crossfield approach, this included dendritic, star and comb polymers. The specific purpose of this work was to: Investigate the effect of star-branching on zero shear viscosity. Investigate the UV-curing performance of star-branched polymers. Synthesize comb-branched polymers and evaluate the film properties of the pure resin and blends with conventional resins. Develop a polymer better suited for a low temperature curing thermoset resin, i.e. with a Tm and Tg proving storage stability and good film properties. Evaluate a series of dendrimers with different cores and terminal groups utilizing a triple detection SEC. 1 2. Background This chapter briefly reviews the areas of interest covered by this thesis. First the basic concepts, applications, and problems associated with powder coatings are introduced. This is followed by a presentation of the different polymerization techniques utilized to synthesize branched polymers. Finally, there is a review of the various macromolecular architectures and their rheological behavior. 2.1 Powder Coatings Powder coatings in their powder form can be either thermoplastic or thermosetting. The first powder coatings, developed in the 1950’s, were thermoplastic and were applied to preheated metal substrates.1 Thermoplastic powder coatings, by definition, are melted to form a film at elevated temperature and solidify upon cooling. Film formation is a result of the melting and coalescence of powder particles. In order for thermoplastic powder coatings to achieve good mechanical properties, high molecular weight of the resin is required. Coalescence and leveling are mainly surface tension driven and the level of viscosity the main property affecting the rate of film formation.2,3 The manufacture of thermoplastic powder coatings is relatively simple and raw materials are normally commodity polymers with overall acceptable properties such as polyvinyl chloride, polyolefines, nylons and polyesters.4 The main disadvantages with these coatings are high fusion temperature, low pigmentation levels, and poor adhesion to metal substrates. In spite of these general shortcomings, some of them display outstanding properties such as solvent resistance (polyolefines), outstanding weathering resistance (polyvinylidene chloride) and exceptional abrasion resistance (nylon). Low price and ease of handling are other advantages.2,5 A few years after the development of thermoplastic powder coatings, Shell Chemicals developed the first thermosetting powder coatings. During film formation of traditional thermosetting powder coatings, a thermally activated reaction takes place, resulting in the formation of a cross-linked polymer. Their introduction solved many of the problems associated with thermoplastic powder coatings. In the late 1960’s and early 1970’s when new laws and regulations in industrialized countries gave powder coating technology a “bump” forward. The main components of thermosetting polymers are a primary resin and a cross-linker.4 Film formation is traditionally accompanied by chemical cross-linking (curing) that commences when the system is heated. Curing affects both the viscosity and the flow. Caution must be taken so that curing does not restrict film formation and leveling, i.e. curing must start well above the glass transition temperature (Tg) of the resin. During curing a threedimensional network is formed by the low molecular weight resin and the cross-linker. Network formation is dependent on the average degree of functionalization of the resin/crosslinker system. It is therefore necessary to control the degree of functionalization (fn), Tg and the number average molecular weight (Mn) in order to obtain the desired network.6 If fn is equal to or slightly over two, the final structure, after full conversion, will be a high molecular weight linear or branched polymer which may have good mechanical properties but poor solvent resistance. On the other hand, if fn is too high, the final structure will have excessive cross-link density and may be brittle with poor mechanical properties. Systems can be tailored to obtain desired properties by changing the chemical structure and cross-link density. Powder coating formulation can be difficult since a number of their properties have conflicting needs: (1) minimization of pre-mature cross-linking during production; (2) 2 stability against coalescence during storage; (3) coalescence, degassing, and leveling, i.e. film formation, at the lowest temperature possible; and (4) cross-linking at the lowest temperature possible.4 Coalescence of the powder during storage can be avoided if the resin has a high Tg. On the other hand, a low Tg allows coalescence and leveling at a lower temperature since the rule of thumb is that the lowest feasible curing temperature is 70-80°C above the Tg of the powder. Viscosity controls the flow and leveling of a powder coating. A low viscosity promotes leveling while a high viscosity impedes leveling. The main driving force for leveling is the surface tension, which is similar for most resins. Of the remaining parameters affecting leveling, such as mean film thickness, and particle size, shape and distribution, viscosity is the only parameter controlled by molecular architecture, weight, and chemical composition. During leveling the shear rate is very low.3,4,7 Thus, the zero shear viscosity critically influences leveling. Over the years the terminology of the different systems has grown and become confused. For clarity, table 2.1 shows some of the major classes of powder coatings along with some details about each. Table 2.1 Overview of the most common powder coating systems.5 Common name Primary resin Cross-linker Curing temp. (°C) Epoxy Bis-phenol A epoxy Polyamines, anhydrides or phenolics 1808 Hybrid COOH-functional polyester Bis-phenol A epoxy 160-2005 COOH-functional polyester Triglycidylisocyanurate or hydroxyalkylamin OH-functional polyester Blocked-isocyanate or amino acid Epoxy-functional acrylic Dibasic acid OH-functional acrylic Blocked-isocyanate or amino resin Acrylate-functional resin Free radical 1205 Epoxy-functional resin Cationic 1209 Polyester Acrylic UV*-cure 180-20011 130-1805 * Ultra Violet The main advantages associated with powder coatings compared to solvent- or water-borne coatings include: near zero volatile organic emission, high application speed, reduced energy consumption, easy clean-up, recycling of over spray (>95% utilization), durable finishes, possibility to apply thick films, and electrostatic application of 3D substrates. The powder coating system also requires less skill and training to operate, substantially reduced flammability and low toxicity.2,10,11,12These advantages have led to continuous growth of the 3 powder coating market during the last few decades. However, powder coatings do have some limitations, namely: increased risk of dust explosions, inability to coat large or heat sensitive substrates, some appearance limitations, major components must be solid which results in material limitations, low production and application flexibility due to the clean-up needed between color changes.4 In addition, the application techniques of thermoplastic and thermoset powder coatings are commonly fluidized bed and electrostatic spray, respectively, thus limiting their use to industrial settings.10 2.1.1 UV-Cured Powder Coatings Traditionally, the powder coating cross-linking reaction has been controlled by temperature. Normal curing temperatures are 160-200°C, and are thus not suitable for application on heat sensitive substrates such as wood and plastic. Curing temperature is determined by the combination of storage stability and the film formation process. Powder coatings must be storable at 30°C without the resin particles fusing, thus the glass transition temperature, Tg, of the polymer must be 60°C or higher. Film formation for amorphous resins requires a temperature at least 50°C above Tg, giving a minimum curing temperature of about 110°C.13 One way to lower the curing temperature is by the introduction of semi-crystalline material with a suitable melting temperature.14 The advantage of using a crystalline resin is the rapid melting, versus the slow softening of an amorphous resin (figure 2.1). Heat Onset of Cure Leveling/ Curing Leveling/ Curing Thermally Cured System Leveling UV-curing UV Cured System Figure 2.1 Film formation process for a thermally cured system (left) versus an UV cured system (right). The UV-curing allows for greater control due to the nature of initiation of cross-linking. Aside from having the appropriate resin, low curing temperature also requires an initiating system that can be activated at low temperatures while stable at room temperature. This is difficult to achieve with conventional thermal initiators, which normally obey an Arrhenius relationship with respect to reaction rate as a function of temperature. One alternative is for 4 the onset of cure to be controlled by the use of ultra violet (UV) initiation, which may result in smoother coatings when desired (figure 2.2). In recent years UV-curing of powder coatings has obtained increased attention in industrial research11,15 as this technique allows fast curing at lower temperatures than conventional powder coatings.16 The research was triggered by the possibility of coating heat sensitive substrates. Other advantages include shorter cycle times, improved storage stability, no premature reaction during manufacturing, and better leveling since viscosity does not increase until UV-irradiated.10 Film formation can be performed at low temperatures (90-140°C) and cured in a matter of seconds with UV.4,10 Although UV-curing offers many advantages, it does have limitations such as working film thickness, interferences due to UV absorbance by pigments, and difficulty in curing complex shapes.10 Though pigmented coatings can be cured, the clear coatings are the most interesting. Powder coatings with bis phenol A epoxy as the binder are cationically UV cured. Acrylated epoxy resins, with or without acrylated polyesters or unsaturated maleic resins as binders, are cured via a free radical mechanism. Log(Viscosity) Crystalline resin UV-cured Amorphous resinthermally cured Onset of UV-cure Temperature/Time Figure 2.2 A schematic diagram of viscosity as a function of temperature/time for a thermally cured amorphous resin and an UV-cured crystalline resin. The onset of cure can be controlled when using an UV-curing system while the thermally cured system starts to cure almost immediately. 5 2.2 Branched Polymers There are a many different types of branched polymers. Dendritic (extremely branched), pom-pom, H-, comb- and star-branched polymers are just some examples. Due to the complex architecture of branched polymers, their properties differ from their linear counterparts. The rheological properties of branched polymers have been studied extensively, especially the star polymers where they have served as models to increase the general understanding of branched macromolecules. 2.2.1 Dendritic Polymers Dendritic polymers, comprised of dendrimers and hyperbranched polymers (figure 2.3), are synthesized from ABx monomers. An ABx monomer consists of two different functional groups, A and B, where there are two or more B’s for every A (figure 2.4). The final structure is dependent upon the growth process. A controlled growth yields a dendrimer while an uncontrolled growth yields a hyperbranched polymer. Dendrimer Hyperbranched polymer Figure 2.3 Schematic representations of a dendrimer and a hyperbranched polymer. 2.2.1.1 Dendrimers The term “dendrimer” was first coined by Tomalia et al. to describe a large family of regularly branched poly(amidoamines).17 Dendrimers contain bonds that converge to a single point with each repeating unit containing a branch junction and with the final molecule featuring a very large number of identical chain ends (figure 2.3). The interest in dendrimers is driven by their possibly unique rheological, mechanical and compatibility properties.17,,18,19 Dendrimers are synthesized under controlled conditions and display a perfect branching pattern. The divergent and convergent growth approaches are the two different stepwise procedures used to synthesize dendrimers. In the divergent growth approach, successfully employed by Tomalia et al.17,18 and Newkome et al.20, the ABx monomers are added layer by layer (or generation by generation) to a multifunctional core molecule. This process leads to larger and larger dendritic molecules with an ever-increasing number of chain ends and functional groups. The convergent growth approach, developed by Hawker and Fréchet21, begins at the chain end and proceeds inwards through successive additions of dendritic 6 molecules to a single building block. In a final reaction, the completed dendrons or arms are attached to a multi-functional core. While it has been shown that the two approaches can give exactly the same structure, the growth process are essentially opposite. One disadvantage of the divergent approach is that it generates a large number of functional end groups which may not all react to form the next completely substituted layer (generation). This makes separation of fully functionalized and almost fully functionalized species impossible. On the other hand, the convergent growth approach offers better control over each step of the synthesis. With each reaction, fewer functional groups are involved and purification is simplified due to the large differences in molar mass between product and by-products. Multiple synthetic steps are required to produce high molecular weight polymers with either approach making the synthesis of dendrimers tedious and expensive. However, recently Fréchet et al. developed a method for the divergent synthesis of aliphatic polyester (bis-MPA) dendrimers utilizing an anhydride building block.22 This approach proved to be highly efficient and circumvented the previous time-consuming purification problems. 2.2.1.2 Hyperbranched Polymers The main features distinguishing hyperbranched macromolecules from dendrimers are the ability to synthesize these structures in one step and that they contain linear units. The linear units produce characteristics such as broad molecular weight distribution and irregular branching (figure 2.4). Hyperbranched macromolecules, first reported by Kim and Webster23, have been studied in detail since 1989. However, Flory discussed the fundamental concepts underlying their synthesis more than 40 years ago.24 Flory predicted that ABx monomers with one reactive group of type A and x reactive groups of type B would polymerize readily and give a soluble, easy to process (low viscosity), three-dimensional structure free of cross-links. B Dendritic unit B B B B + Core molecule A B B A B B B B B B B B B B B Terminal unit B Linear unit B B B B B B B B B B B B Core molecule B Figure 2.4 Schematic of the synthesis, structure and different repeating units of a hyperbranched polymer. Hyperbranched macromolecules contain three types of repeating unit dependent on degree of substitution; dendritic, linear and terminal (figure 2.4). The dendritic unit is composed of fully substituted AB2 monomers, the linear unit has one reacted and one unreacted B group, and the terminal unit has two unreacted B groups. The degree of branching (DB), used to characterize hyperbranched polymers, defined by Fréchet et al25, follows: 7 DB = ∑ Dendritic units + ∑ Terminal units ∑ All repeating units Dendrimers have a DB of 1 since they contain only dendritic and terminal units. The comparison of two hyperbranched polymers with the same chemical composition but different DB has shown that solubility increases with the degree of branching while the melt viscosity is inversely related.26 Hyperbranched polymers are usually prepared in a single-step polymerization and are thus not as tedious to synthesize as dendrimers. Even though theoretically one-step growth of a hyperbranched macromolecule could lead to a “perfect” dendrimer, it has never been encountered due to the kinetics of the polymerization techniques used. A living polymerization may lead to more dendrimer-like structures. To obtain a high molecular weight hyperbranched polymer, several conditions must be fulfilled e.g. the reactive groups, A and B, should only react with each other and side reactions should be kept to a minimum preventing deactivation and cross-linking.27 Hult et al.28 used p-toluene-sulfonic acid to catalyze the bulk synthesis of hyperbranched aliphatic polyester in the molten state. 2,2Bis(methylol)propionic acid (bis-MPA) was used as the monomer and 2-ethyl-2(hydroxymethyl)-1,3-propanediol as the core molecule. Voit et al. have performed additional work with the same monomer.29 2.2.2 Star-Branched Polymers Star polymers are one of the simplest forms of branched polymers. They consist of a core molecule onto which linear polymers are coupled or grafted from. Synthesis can be divided into three general approaches described in figure 2.5. The first route is the core-first method where polymer chains are grown directly from a multifunctional core (route A). The other two routes utilize the arm-first method, where preformed linear polymers are linked to a multifunctional coupling agent or a diene (routes B and C).30 One of the most common approaches is anionic polymerization of monodisperse arms, then attachment to a chlorosilane functional core molecule, which can vary in degree of functionalization (route B), permitting good control of molecular weight and polydispersity.31 Other synthetic approaches include atom transfer radical polymerization,32,33 nitroxidemediated polymerization,34 ring-opening polymerization (ROP) utilizing coordination insertion,35 ring-opening metathesis polymerization36 and radical addition-fragmentation chain-transfer polymerization.37 Some of the uses for star polymers include various coating applications such as antifouling coatings, conductive coatings and low volatile organic content coatings.38,39,40 Star polymers are also used as colloidal stabilizers, additives to improve impact resistance and reduce permeability, and in medical/surgical devices.41,42,43 8 Monomer Multifunctional initiator + Living prepolymer Multifunctional core moiety R + Living prepolymer Diene Polymerization Coupling reaction Linking reaction A B C Figure 2.5 Schematic illustrations of the three approaches for the synthesis of a starbranched polymer. 2.2.3 Comb-Branched Polymers Comb-branched polymers consist of a backbone with polymer side chains.44 The backbone and side chains can either be of the same or different chemical composition (graft copolymers). Some of the first graft copolymers were acrylonitrile-butadiene-styrene copolymer (ABS), high impact polystyrene (HIPS) and non-ionic emulsifiers. In the case of ABS and HIPS, the copolymerization yielded a better result than merely physical blending due to the low compatibility between the components.45,46 The synthetic approaches for comb polymers are the same as for star polymers. 2.3 Ring-Opening Polymerization Ring-opening polymerization (ROP) can proceed through a number of different mechanisms depending on the type of monomer and catalyst involved. Of the wide range of polymers produced via ROP, some have gained industrial significance; for example poly(caprolactam) and poly(ethylene oxide).47 ROP of cyclic esters, such as ε-caprolactone (CL) and L,L-dilactide, is gaining industrial interest due to their degradability.48 The mechanisms of interest of interest in this work are coordination insertion and cationic. 9 2.3.1 Coordination Insertion Ring-Opening Polymerization Coordination insertion ring-opening polymerization is an effective route to obtain welldefined polyesters. Stannous(II) 2-ethylhexanoate (Sn(Oct)2) is a common catalyst for the ROP of lactones and lactides.49 There are two main proposed mechanisms for the ROP of cyclic esters using Sn(Oct)2 and a hydroxyl functional co-initiator; complex formation between the monomer and hydroxyl group prior to ROP and formation of a tin-alkoxide prior to initiation.50,51 The main advantage of ROP of cyclic esters (and amides) versus a condensation reaction of the equivalent hydroxy carboxylic acid is absence of water formation. 2.3.2 Cationic Ring-Opening Polymerization A broad range of heterocyclic compounds can undergo cationic ring-opening polymerization (CROP).48 CROP propagates either through an activated monomer or an activated chain end mechanism. In both cases the propagation involves the formation of a positively charged species.52 A major drawback of CROP is the occurrence of unwanted side reactions, thus limiting the molecular weight of the final product.53,54 2.4 Rheology in the Molten State Rheology is defined as the science of the deformation and flow of matter. In the molten state linear polymers often exhibit pronounced viscoelastic properties, such as shear thinning, extension thickening, viscoelastic normal stresses, and time-dependant rheology. All of these properties are due to the physical nature of most polymers, which is long and easily distorted. Viscosity is a measure of a fluid’s resistance to flow and describes the internal friction of a moving fluid. Viscosity is an extremely important property of polymer melts and solutions since it controls the possibility of processing. If the viscosity is too high, processing will be difficult or impossible. In the case of powder coatings (and other types of coatings), viscosity controls leveling. 2.4.1 Rheological Behavior of Linear Polymers The main factor affecting viscosity in the molten state is the molecular weight. Figure 2.6 shows the well-known plot of how zero shear viscosity (η0) relates to molecular weight (M).55 η0 depends on M as η0 ∝ M below the critical molecular weight (Mc) and η0 ∝ M3.4± 0.1 above Mc. 10 Log(η0) η0∝M3.4 η0∝M1 MC Log(M) Figure 2.6 The relationship between zero shear viscosity (η0) and molecular weight (M) for a linear polymer with low polydispersity. The steep increase in viscosity above Mc is due to entanglements. Entanglements restrict molecular motion by preventing chains from passing one another and moving perpendicular to their own molecular contour. In order to relax stress, individual polymer chains have to move along their own contour in a snake-like fashion. This snake-like motion is called reptation.56 For linear polymers the onset of entanglement starts at their Mc, which for highly flexible polymers ranges between 300-600 atoms in the main chain.57 2.4.2 Rheological Behavior of Branched Polymers Dendritic polymers are essentially free of entanglements and exhibit a spherical shape at higher generations due to sterical and branching considerations. This results in unique rheological properties, which is one of their most prominent features.58,59 In contrast to chaintype macromolecules, which exhibit a non-Newtonian shear thinning behavior at a critical shear, dendritic macromolecules exhibit Newtonian flow behavior in solution and bulk regardless of the number of generations.60 The rheological properties of star-branched polymers have also been extensively investigated. Due to their simplicity, they have served as models for the development of new or refinement of existing rheology theories.61,62 The rheological behavior of star polymers differs from linear and dendritic polymers, since their relaxation modes are different. Entangled star polymers cannot relax through reptation since one end is attached to a core moiety. The arms relax through primitive path fluctuations63,64 and constraint release.65 During primitive path fluctuations, some times called “breathing modes”, a polymer arm is drawn back and then re-extended into a new tube. Constraint release occurs when surrounding arms fluctuate. Tube widening by constraint release is analogous to the addition of a low molecular weight solvent and is therefore called “dynamic dilution”.66 As previously mentioned, η0 depends on M as η0 ∝ M below Mc and η0 ∝ M3.4 above Mc. However, for star polymers the viscosity increases exponentially with molecular weight67 and hence no Mc is found to coincide with the onset of entanglement. Also, the η0 of a star polymer is not dependent on the total M, but on the arm M.68 This makes it possible to 11 increase the molecular weight without changing the viscosity by increasing the number of arms. Comb polymers are normally less defined than star polymers but studies have shown that the η0 of comb polystyrenes is lower than that of a linear polymer with the same molecular weight.69,70 In addition, Sherrington et al. prepared a large number of branched poly(ethylene terephthalate)s (PET) by addition of a branching agent and a chain stopper. The branched PET’s exhibited both lower solution and melt viscosities in spite of a significantly higher molecular weight than the linear model polymer.71 12 3. Syntheses and Chemical Characterization This chapter covers the synthesis and chemical characterization of the different branched polymer structures, which appear in this work. The chemical characterizations include nuclear magnetic resonance (NMR), size exclusion chromatography (SEC), Fourier-transform infrared spectroscopy (FT-IR) and FT-Raman. Triple detection (SEC3) and universal calibration (SECUC) were utilized in the SEC characterization. Also covered in this chapter is the SEC characterization of a series of dendrimers. 3.1. Monomers The monomers used as the starting material in the synthesis of the different architectures are shown in figure 3.1. 2,2-Bis(methylol)propionic acid (bis-MPA), a crystalline dihydroxy carboxylic acid, was used as the monomer in the synthesis of the dendron and dendrimer. It is also the monomer for the hyperbranched polymer Boltorn H-30 (commercially produced by Perstorp).72 ε-Caprolactone (CL), a liquid cyclic ester, was used to synthesize the arms of both the star-branched and comb poly(ε-caprolactone)’s (PCL). 5,5-Dimethyl-1,3-dioxane-2-one, also known as neopentyl carbonate (NPC), was the crystalline cyclic carbonate used in the synthesis of the star-branched poly(neopentyl carbonate) (PNPC). The hydroxyl functional initiators used in the synthesis of the PNPC stars and the comb polymer backbone are not included in figure 3.1, however the structures of the initiators are described in section 3.3.1.2 and the composition of the backbone is described in section 3.4. O OH O O O HO O O OH Bis-MPA ε-Caprolactone Neopentylene carbonate Figure 3.1 Monomers used in the synthesis of the various macromolecular architectures. 3.2 Star-Branched Poly(ε-caprolactone)’s Variations were made in the architectures of a group of star-branched PCL’s in order to investigate the effect of branching on zero shear viscosity. ε-Caprolactone was chosen as the monomer due to its ease of polymerization and to the semi-crystallinity of the formed polymer. 13 3.2.1 Synthesis The synthesis of star polymers can be divided into three parts: synthesis of the core molecules, grafting, and end capping. The core molecules include the third generation bisMPA dendron and dendrimer which were synthesized according to a procedure by Hult et al.73 The final core moiety was a pseudo third-generation, bis-MPA based, hyperbranched molecule, similar to a polymer developed by Hult et al.,28,74now commercially available under the trade name Boltorn and kindly supplied by Perstorp AB. Grafts were accomplished by ring-opening polymerization (ROP) of CL onto hydroxyfunctional cores. The reactions were performed in bulk at 110°C with Sn(Oct)2 as the catalyst with the degree of polymerization (DP) controlled by the monomer to initiator feed ratio. Finally, the hydroxy-functional end groups of poly(ε-caprolactone) (PCL) were end-capped with methacrylate groups (scheme 3.1). HO OH OH HO O OH + HO OH HO OH Sn(Oct)2 110°C O OH HO HO O n OH O O O O HO O O O O O nO O O O O O n OH O O nO O O n O O O O O n O O O O HO n O O O n nO O O HO O O OH O n O OH OH Scheme 3.1 General outline of the synthesis of star polymers where the large center circle represents a dendritic core molecule. The final end capping is not included in the scheme. The various star-branched polymers differed with respect to the length of the PCL grafts and the type of core molecule. Throughout, the initiator and monomer were carefully dried, as 14 traces of water would initiate homo-polymerization. The structures of the different star polymers are presented in Appendix A. 3.2.2 NMR Characterization The 1H NMR spectra of the polymers were used to calculate the DP of the PCL grafts and the molecular weight (table 3.1). The DP was calculated by comparing the integrals of the protons on the methylene adjacent to the hydroxyl end-group (A) relative to those on the methylene next to the carbonyl carbon (C) (figure 3.2). Although it is also possible to perform the calculation by comparison with the methylene next to the oxygen in the repeat unit (B), this method of calculation is inferior due to the overlapping shift of the core molecules. The accuracy of the DP value obtained for polymers with high DP is reduced due to the reduced relative size of the peak from the protons next to the hydroxyl group. B C 32.5 1.0 Integral 4.1 4.0 3.9 3.8 3.7 3.6 3.5 (ppm) O B C R n O O OH C A A Integral 7.5 32.5 7.0 6.5 6.0 5.5 5.0 4.5 1.0 4.0 3.5 34.6 3.0 2.5 2.0 1.5 1.0 0.5 (ppm) Figure 3.2 1H NMR spectrum of a dendron-PCL with an average DP of about 35. It has been shown that the 13C NMR shift of the quaternary carbon in the repeat unit of the initiating species is sensitive to the degree of substitution.28 This quaternary carbon resonates at 50.6 ppm if both hydroxyl groups are unreacted, at 48.8 ppm if one hydroxyl group remains, and at 46.8 ppm if both hydroxyl groups are reacted. This resonance change is useful in assessing the success of the grafting reaction. 13C NMR spectra of the polymers showed that those with shorter arms still contained unreacted hydroxyl groups (figure 3.3). 15 51 50 49 48 47 46 45 44 (ppm) 13 Figure 3.3 C NMR spectrum of the quaternary carbons from the bis-MPA repeating unit in the hyperbranched core of Boltorn-PCL, DP8. The peak at 46.8 ppm shows the presence of fully functionalized bis-MPA hydroxyl groups. The peak at 48.8 ppm shows the presence of partially functionalized bis-MPA end groups. The absence of a peak at 50.6 ppm shows that there are no end groups with both hydroxyl groups unreacted. The integral calculation of functionalization shows that approximately four hydroxyl groups remain unreacted. (The peaks are shifted downfield 0.8 ppm due to an uncalibrated spectrum.) Full functionalization was observed at varying DP for the various structures analyzed (figure 3.4). The dendron and dendrimer were fully reacted at a DP of about 13-15 while the hyperbranched polymer was fully substituted at a DP of about 20. The spectra further showed that in all cases only one of the hydroxyl groups, 48.8 ppm, was unreacted. This lack of functionalization was probably due to the statistical nature of the reaction since the star polymers with longer arms showed no trace of incomplete functionalization of end-groups. 51 50 49 48 47 46 45 44 (ppm) 13 Figure 3.4 C NMR spectrum of Boltorn-PCL, DP of 32. Only one peak at 46.8 ppm indicates that all hydroxyl groups have reacted. (The peak is shifted downfield 0.8 ppm due to an uncalibrated spectrum.) 3.2.3 SEC Characterization Size exclusion chromatography (SEC) was performed to determine molecular weight and distribution. The SEC apparatus equipped with a triple detector array, including differential refractive index, differential viscometer and right (and low) angle laser light scattering detector (RALLS). This set-up permitted molecular weight to be determined using conventional, universal (SECUC), and triple detection calibration (SEC3), simultaneously.75 16 SECUC is based on the fact that VH ∝ [η]M ,where is the hydrodynamic volume and [η] is the intrinsic viscosity, for a wide range of polymers and complex architectures including e.g. dendritic-, H-, star-, comb- and co-polymers.76,77,78 This makes SECUC a useful tool for the determination of molecular weight since there is no influence from the architecture or chemical composition of the analyzed compounds. The molecular weights, especially the weight average molecular weight (Mw), obtained from SEC3, are in general, very close to those from SECUC, which is to be expected since both methods are independent of architecture and chemical composition. However, light scattering (SEC3 method) is dependent on the refractive index increment, which is low for PCL in tetrahydrofuran (the mobile phase), resulting in poor signal to noise ratio, especially for the low molecular weight fraction. The agreement of the SECUC data with the number average molecular weight (Mn) from 1H NMR data is, in general, good at low DP. This agreement is reduced at high DP since accurate end-group analysis becomes more difficult with increasing DP (table 3.1). In addition, the SEC determination of Mn is very sensitive to errors and difficult o determine exactly. Polydispersity generally increased with increasing molecular weight. This is due to intra- and intermolecular transesterification that occurs at high conversion and molecular weight.79 Table 3.1 SEC and 1H NMR data of the star-branched PCL characterized with SEC3 and SECUC. Mark-Houwink (MH) equation: [η] = kM α . The MH α value is a polymer conformation parameter. The α value decreases with the compactness of the structure. (degree of polymerization DP, polydispersity index PDI) DP aim DP 1 H NMR 1 Mna H NMR Boltorn-PCL 50 51 189 900 70 79 292 200 Dendrimer-PCL 12 14 41 100 15 14 41 100 20 24 68 500 35 42 117 700 60 51 142 300 Dendron-PCL 18 15 14 600 40 46 42 900 80 81 74 900 Linear PCL 15 17 2 200 50 45 5 400 80 82 9 600 A 17 1 900 B 39 4 400 C 117 13 300 a g mol-1 SEC SECUC PDI SEC SECUC MH α value Branching average 239 000 303 800 1.58 1.54 236 300 308 700 9.13 7.86 0.263 0.204 39 46 41 300 42 300 67 300 99 900 109 200 1.44 1.39 1.31 1.60 1.47 42 000 43 700 72 100 104 700 122 300 1.04 1.03 1.01 1.14 1.30 0.771 0.775 0.742 0.758 0.787 18 19 24 22 23 15 800 47 800 68 000 1.27 1.39 1.30 16 000 43 000 66 400 1.01 1.27 1.71 0.822 0.836 0.817 6.8 8.2 8.5 3 000 6 400 13 300 2 800 6 600 16 900 1.23 1.24 1.53 1.20 1.53 1.38 2 300 5 200 10 300 2 200 5 100 14 200 1.01 1.03 1.46 1.02 1.46 1.41 0.888 0.860 0.885 0.865 0.923 0.908 - Mwa 3 PDI 3 Mwa 17 The polydispersity index (PDI) values obtained from SEC3 are similar for all samples whereas there is a broad distribution/range of PDI’s obtained from SECUC. This can be attributed to the insensitivity of the RALLS detector (SEC3) to low molecular weight polymers with a low refractive index increment, resulting in too narrow distribution of the disperse polymers (Boltorn-PCL). In addition, when considering the multifunctional initiator moieties, Boltorn a polydisperse hyperbranched polymer, the monodisperse dendron and dendrimer it is obvious that the SEC3 PDI’s are incorrect. The PDI of Boltorn H-30 in N,N-dimethylformamide and THF utilizing SECUC is, according to a study performed by Månson et al. at least 2.80 The Mark-Houwink (MH) data permits the calculation of the number of arms on a star polymer. Polymers with long chain branches such as star- and comb-branched polymers have reduced hydrodynamic radius and intrinsic viscosity [η] compared to linear polymers of the same molar mass. By comparing the intrinsic viscosity of a branched polymer and a linear reference polymer it is possible to estimate the degree of branching. The number of arms was calculated using the Zimm-Stockmayer equations.81 Through the comparison of the intrinsic viscosity of the branched polymer ([η]b) and a linear equivalent ([η]l), the branching index g is calculated: [η ] g = b [η ]l where ε is a form factor dependent on the type of branched polymer.82,83 The form factor is generally considered to be ∼0.75. This definition of g is less exact than the ratio of the radius of gyration (RG), however it is more practical to use due to the problems associated with measuring RG over the whole molecular weight distribution. The number of arms is then calculated using81 g = (3 f − 2 ) / f 2 1/ ε where f is the number of arms. The calculated number of arms is in good agreement with the theoretical number of arms for the star polymers with a dendron and dendrimer core moieties. Their number of arms is 8 and 24 respectively. At lower DP the measured number of arms is lower than the theoretical value. This was expected since the 13C NMR showed that functionalization at low DP’s was incomplete. The Boltorn-PCL with theoretically 32 arms, however, displayed a higher number of arms. This can be contributed to the nature of Boltorn, a hyperbranched polymer with a lower degree of structural uniformity. Appendix B lists SEC as determined by SECUC and viscosity data of all star-branched PCL. 3.3 Star-Branched Poly(neopentyl carbonate)’s One of the goals of this work was to identify a solid material suitable for low temperature curing. Since the thermal properties of branched poly(ε-caprolactone)’s are unsuitable for applications as solid coatings (Tg = -55°C Tm = 35-50°C). An interesting candidate for this is the polymer of 5,5-dimethyl-1,3-dioxane-2-one or neopentyl carbonate (NPC). The polymer has a reported Tg of 20-30°C and Tm of 100-130°C.84,85,86,87 An additional feature of polycarbonates is increased resistance to hydrolysis compared to polyesters.88 While there are no references of branched poly(NPC) (PNPC) in the open literature, there is at least one claim of a star-branched PNPC that can be found in the patent literature. The patent claims synthesis of stars from NPC and pentaerythritol catalyzed by stannous(II) 2-ethylhexanoate (Sn(Oct)2) although no detailed characterization is disclosed.89 18 3.3.1 Synthesis 3.3.1.1 Monomer Synthesis Preparation of NPC from diethyl carbonate and neopentyl glycol as previously described by Sarel et al.90 References to production of NPC are also found in patent literature.91,92 The reaction proceeded in two steps. In the first step, oligomer or prepolymer was formed which was subsequently subjected to pyrolysis and ring closure resulting in a cyclic monomer. The synthetic route used in this work was similar to the patented procedures in that it omits an extraction step. Sn(Oct)2 was used as catalyst to ensure formation of prepolymer and increase the rate of ring closing depolymerization. All volatile by-products and reagents including residual neopentyl glycol were removed under reduced pressure and NPC was obtained by pyrolysis at 210°C followed by distillation (scheme 3.2). This elaborated method does not require extraction and the monomer could be conveniently prepared in 200 g scale in one pot with a 70% yield. O O OH HO + O Sn(Oct)2,130°C O -EtOH Prepolymer Pyrolysis, 210 °C O O Scheme 3.2 Synthetic route for NPC. 3.3.1.2 Polymer Synthesis An experimental series was designed in order to find favorable conditions for the synthesis of star-branched PNPC’s with cores consisting of various polyols. Polymers with three and four arms were synthesized from trimethylolpropane (TMP) (3OH), di-TMP and etoxylated pentaerythritol (PP50) (4OH). TMP and di-TMP represent polyols with primary hydroxyl groups in neopentylic positions. PP50, on the other hand, has approximately 5 ethylene oxiderepeating units per molecule and the hydroxyl groups in this polyol are less sterically crowded. Star-branched polymers were also synthesized from a Boltorn H30 (3rd pseudo generation) (Appendix C). In addition, linear PNPC by initiation from n-BuOH was synthesized and used as a reference compound. HO HO OH HO HO O O OH OH TMP OH O OH O OH Di-TMP O O HO PP50 Figure 3.5 Three and four functional core molecules. Previously reported work suggests tin(II) compounds and mild organic acids as promising catalysts for realization of the target structures. Kricheldorf et al. reported the synthesis of 19 linear PNPC with a molecular weight of up to 250 kg mol-1 by a coordination insertion mechanism utilizing Sn(Oct)2.85 Hedrick et al. have reported stannous(II) trifluoromethane sulfonate (Sn(OTf)2) as an efficient catalyst for polymerization of lactones under milder conditions than Sn(Oct)2.93 NPC has also been polymerized cationically. There are two proposed mechanisms, the activated monomer mechanism and the activated chain end mechanism. Early work on cationic polymerization of NPC reports side reactions causing decarboxylation that result in formation of ether groups in the growing chains. Reported initiator systems consist of strong acids, such as triflic acid or boron trifluoride,86,94,95 and more recently living systems, such as triethyl borate/HCl.Et2O.87 However, the use of strong acids can increase the risk of side reactions during polymerization, and the nature of the alkyl borate initiating species prevents initiation from a multifunctional scaffold. The catalysts chosen for this study were Sn(Oct)2, Sn(OTf)2 and fumaric acid (pKa= 3.02). The choice of fumaric acid was inspired by the work of Endo et al. who recently synthesized ε-caprolactone star-branched polymers utilizing this catalyst.96 3.3.2 NMR Characterization 1 H NMR was employed to monitor conversion and estimate the degree of polymerization (DPNMR) (figure 3.6). Conversion was calculated by comparing the peak integral at 1.12 ppm (b) with the peak at 0.99 ppm (b’). The peak 1.12 ppm (b) corresponds to the protons of the methyl groups in the monomer and the peak at 0.99 ppm (b’) represents the methyl groups of the polymer backbone. The DPNMR was calculated by comparing the integrals of the repeating unit peak at 0.99 ppm (b’) and the peak at 0.93 ppm (d), corresponding to the methyl groups in the terminal repeat unit. The DPNMR is thus equal to I0.99/I0.93+1. This calculation can also be performed on the integral at 3.34 ppm (c) that corresponds to the CH2 in the α position to the terminal hydroxyl group. In this case DPNMR is equal to I0.99/(3×I3.34)+1. If di-TMP is present as the initiating polyol, the protons located next to the ether bond in di-TMP yield a resonance peak in the vicinity of 3.3 ppm, which makes it impossible to calculate DP using the peak integral at 3.34 ppm (c). However, the peaks arising from the ether bond in di-TMP indicate where peaks would likely emerge if ether bonds were formed during the polymerizations. Since decarboxylation and the formation of undesirable ether bonds is known to occur in cationic polymerization of cyclic carbonates.86,95 The fact that the integral of the 3.3 ppm resonance peak did not increase during the polymerization from di-TMP and it was not found in any of the other prepared polymers, it is evident that no ether bonds were formed during polymerization. 20 O R O O a´ O O c O n b´ O H d b´ a´ O a O O b a 6.5 6.0 5.5 5.0 4.5 d HBP Boltorn Boltorn HBP 7.0 b c 4.0 3.5 3.0 2.5 2.0 1.5 1.0 0.5 (ppm) Figure 3.6 1H NMR spectra of a Boltorn-PNPC containing unreacted monomer. The degree of substitution of the hydroxyl groups of Boltorn was investigated using 13C NMR. As previously mentioned, Hult et al. have shown that the 13C NMR resonance corresponding to the quaternary carbon of the bis-MPA repeat unit is dependent on the degree of substitution.28 The resonance shifts for the fully substituted, mono-substituted and unsubstituted Boltorn are 46, 48 and 50 ppm respectively. A distinct peak was detected at 46 ppm accompanied by a smaller peak at 48 ppm, suggesting that the majority of the hydroxyl groups of Boltorn were substituted (figure 3.7). 50 48 46 (ppm) 160 150 140 130 120 110 100 90 80 70 60 50 40 30 20 10 (ppm) Figure 3.7 13C NMR spectra of a Boltorn-PNPC. The enlarged area shows the quaternary carbons. 21 3.3.3 SEC Characterization A universal calibration (SECUC) method was used to study the obtained star polymers while triple detection including light scattering was excluded due to a poor signal to noise ratio. All polymers were synthesized using fumaric acid as the catalyst. The relationship between intrinsic viscosity the degree of branching is discussed in section 3.2.3. This relationship can also be used to rank polymers according to branching by comparing the Mark-Houwink (MH) plots of the respective polymers.97,98 The MH plots for linear, 4-arm and multi-arm star-branched polymers are depicted in figure 3.8. A trend is clearly seen with decreasing slope in the order linear, four arm and multiarm polymer. This suggests successful grafting of PNPC onto the multifunctional initiator molecules. -0.25 PP50-PNPC 4 arm star -0.59 -0.92 Hyperbranched Boltorn-PNPC -1.26 Linear -PNPC -1.60 2.91 3.26 3.62 3.98 4.34 4.69 5.05 Relative response Log[M] Figure 3.8 Mark-Houwink plot of linear and star-branched PNPC. 9.0 13.0 17.0 20.0 Retention volume (mL) Figure 3.9 SEC traces of PNPC polymerized from Boltorn (left), PP50 (center) and n-BuOH (right). The SEC traces of the same polymers are shown in figure 3.9. The Boltorn-PNPC is bimodal, most likely linear or polymers with a few arms; this can be seen in the figure 3.8 in 22 that the low molecular weight region has a different slope. The four arm star and the linear polymers are unsymmetrical, an indication of side reactions. 3.3.4 Catalyst Evaluation Linear PNPC initiated from n-BuOH were synthesized in order to evaluate the catalytic performance of Sn(OTf)2 in toluene under mild conditions. The degree of polymerization (DP) controlled by the monomer to initiator feed ratio The DP aimed for (DPaim) were 20 and 100. The polymerizations were performed in toluene at 50°C in order to prevent n-BuOH from boiling. The polymerizations were run to 90% conversion; the yields after precipitation in cold methanol were 70 and 60% for the DPaim 20 and 100 respectively (table 3.2). The low yield is the result of side reactions that result in a fraction of soluble oligomers, and this decrease in yield was most evident at the higher monomer to initiator ratio. The SEC trace was bimodal at the high DPaim with moderate PDI in both cases. The efficiency of the catalysts to form star polymers was evaluated by reacting NPC with diTMP in presence of the respective catalysts: Sn(Oct)2, Sn(OTf)2 and fumaric acid (table 3.2). The polymerizations were performed in bulk at 130°C in order to maintain low viscosity at high conversions. The polymerizations utilizing Sn(Oct)2 and Sn(OTf)2 exhibited high PDI’s, indicating poor control. The PDI was significantly lower for the polymer synthesized using fumaric acid. As fumaric acid resulted in the lowest PDI it was selected for further study. A linear relationship between conversion and molecular weight was observed for conversion up to 80-90% (figure 3.10). Polydispersities were fairly low (1.2) at conversions below 50% and increased gradually up to 2-2.5 above 90% conversion. The observed increase in Mw and broadening of PDI show an increase in side reactions at high conversion. However, observed side reactions in this reaction were significantly lower than observed for the tin catalysts (table 3.2). All polymerizations showed Mn values lower than the theoretical values. The deviation of Mn from the theoretical value was greater at higher DP’s, and may to some extent be attributed to spontaneous thermal polymerization or initiation from impurities. An experiment was therefore performed to determine the extent of thermal polymerization or decomposition of monomer; NPC was heated at 130°C for 24 hours resulting in 6% conversion according to 1H NMR. 6000 2 1.9 Mn, NMR Mn, SEC PDI 4000 1.8 1.7 1.6 3000 1.5 PDI Mn (g mol-1) 5000 1.4 2000 1.3 1.2 1000 1.1 0 0 20 40 60 80 1 100 Conversion (%) 1 Figure 3.10 Mn obtained from H NMR, SEC and PDI as a function of conversion for the polymerization of NPC with a DPaim of 40 by fumaric acid at 130°C. 23 Table 3.2 Data of the ROP of NPC with hydroxyl functional initiators in the presence of different catalysts. a Initiator Catalyst DPaim n-BuOH n-BuOH Di-TMP Di-TMP Di-TMP TMP TMP PP50 PP50 Boltorn Boltorn Boltorn** Boltorn Sn(OTf)2 Sn(OTf)2 Sn(Oct)2 Sn(OTf)2 Fumaric acid Fumaric acid Fumaric acid Fumaric acid Fumaric acid Fumaric acid Fumaric acid Fumaric acid Fumaric acid 20 100 10 10 10 5 20 10 20 5 10 10 30 Mna theo. 2 700 13 100 5 400 5 400 5 400 2 100 7 800 5 600 10 700 23 000 42 000 42 000 120 000 Temp. (°C) 50 50 130 130 130 130 130 130 130 130 130 130 130 Time (h) 48 48 16 4 9 5 9 9 20 4 6 24 24 Conv. (%) 93 91 85 90 70 83 47 75 90 73 80 80 92 Yield (%) 70 60 60 70 55 68 35 60 75 * 65 - 75 g mol-1. * No precipitation. ** Data in this row is from a fractional precipitation of the sample above it. 24 Mna NMR 1 800 2 100 4 700 4 800 3 400 1 900 3 400 3 900 7 600 22 000 30 000 30 000 47 000 Mna SEC 2 400 3 800 4 700 4 900 3 100 1 800 3 400 4 700 6 600 8 500 25 000 4 000 Mna SEC 2 700 4 700 18 400 13 800 4 300 2 900 4 500 6 000 9 000 52 000 99 000 20 000 PDI α 1.2 1.2 3.9 2.8 1.4 1.6 1.3 1.3 1.3 6 4 5 0.69 0.70 0.43 0.30 0.39 0.30 0.12 0.46 0.46 0.12 0.28 0.12 The polymers derived from PP50 showed lower polydispersities at high conversion (90%) compared to polymers based on initiators with neopentylic hydroxyl groups (table 3.2). The SECUC values obtained for the three and four arm star polymers were close to those obtained by 1H NMR. Polymerizations initiated from Boltorn in the presence of fumaric acid had aliquots taken for 1H NMR analysis. The analysis of synthesis with a DPaim of 10 showed that the molecular weight increased up to a DP of 7-8. Additional polymerizations were performed with DPaim of 5, 10 and 30. Conversions were kept below 90% to avoid gelling. 3.3.5 Thermal Characterization The precipitated polymers were subjected to differential scanning calorimetry (DSC) analysis that comprised two melting/crystallization cycles with heating and cooling rates of 10°C/min. In the first cycle the sample was heated from 25 to 140°C and then cooled to 30°C. The sample was then heated to 140°C to complete the procedure. On the second heating, melting endotherms were only observed for three and four arm star polymers with an arm length of 8-10 repeating units or more (figure 3.11). A one-hour annealing segment at 50°C was therefore added prior to the second heating but no or little effect was observed. A Tg was also observed between 20-30°C. Some endotherms were bimodal or very broad on the second heating. Boltorn-PNPC DPaim=30 was the only multiarm star that exhibited an endotherm in the second heating. The two distinct melting endotherms that may be attributed to the presence of linear polymer (figure 3.11). Endo Linear PNPC Di-TMP-PNPC PP50-PNPC Boltorn-PNPC -50 0 50 100 150 Temperature (°C) Figure 3.11 DSC traces for linear and star polymers, 2nd heating after annealing 50°C, 1 h. 25 3.4 Comb-Branched Poly(ε-caprolactone)’s The comb-branched polymers were synthesized as complement to the star-branched polymers. The following study of the comb polymers included investigation of the performance as a powder coating and the overall effect of varying the architecture. 3.4.1 Synthesis The comb polymers were synthesized from a backbone, ER 065. ER 065 is a polyacrylate resin obtained from BASF AG, or more specifically, a copolymer consisting of 20 wt.% glycidyl methacrylate, 5 wt.% of butyl acrylate, 55 wt.% methyl methacrylate and 20 wt.% styrene. The oxirane group of glycidyl methacrylate provided the reactive site for the first reaction with bis-MPA, creating the hydroxyl functional resin (HR) necessary for the ROP of CL. The reaction between oxirane and bis-MPA was not only convenient but also efficient since the procedure was merely a melt mixing (155°C) of the components and the catalyst, tetrabutyl ammoniumbromid (TBAB). In addition, this reaction increased the functionality since each oxirane group was reacted with bis-MPA, which has two hydroxyl groups (Scheme 3.3). n O O n O + O HO O 1wt% TBAB, 155 °C HO OH OH O O O OH OH O O , Sn(Oct) , 110 °C 2 O O HO mO O O HO O O O O O O m m =10 or 20 O O O n HO , TEA, DMAP O O O O O mO O O O O O m O O O O O HO n O Scheme 3.3 Synthetic scheme of a comb polymer. (tetrabutylammoniumbromid-TBAB, triethylamine-TEA, N,N-dimethylaminopyridine-DMAP) 26 The PCL side chains were grafted onto bis-MPA and end-capped using the procedure described for star-branched PCL in section 3.3. The different comb polymers and their precursors are presented in table 3.3. Table 3.3 A list of the different resins synthesized and tested. The resins were polymerized and end-capped batch wise (B = batch). Description Resin ER 065 HR Comb-PCL10, B1-B4 Comb-PCL20, B1-B4 Comb-PCL10M, B1-B2 Comb-PCL20M, B1-B2 Starting material, epoxide functional amorphous resin ER 065 functionalized with bis-MPA, hydroxy functional ε-Caprolactone polymerized from HR, DPaim=10 ε-Caprolactone polymerized from HR, DPaim=20 PCL10 end capped with methacrylic anhydride PCL20 end capped with methacrylic anhydride 3.4.2 IR Characterization The reaction between oxirane and bis-MPA was monitored with FT-IR and FT-Raman99,100 spectroscopy (FT- Fourier Transform). Samples were taken every five minutes until the reaction was complete. Figure 3.12 shows the FT-IR spectra of the individual components, ER 065 and bis-MPA, and allowing their comparison with the reaction mixture after 30 minutes. The carboxyl acid peak of bis-MPA shifts from 1683 to 1721 cm-1. This shift corresponds to the formation of an ester, i.e. the same shift as the acrylate carbonyls. The broad hydroxyl signal at 3200–3600 cm-1 of bis-MPA is decreased due to the low concentration of bis-MPA in the final reaction mixture (85 wt. % ER 065 + 15 wt. % bis-MPA). 1722 701 1136 759 ER 065 989 1452 907 843 1384 2949 1023 1683 630 1232 1044 996 935 868 3358 A 1306 Bis-MPA 2946 1141 908 790 1455 1386 1721 1138 701 759 Reaction mixture after 30 minutes 2948 4000,0 3600 3200 2800 2400 2000 1800 cm-1 988 1452 842 1385 1600 1400 1200 1000 800 600,0 Figure 3.12 IR spectra of ER 065, bis-MPA and of the reaction mixture, 85 wt.% ER 065 and 15 wt.% bis-MPA, after 30 minutes. After 30 minutes the peak at 1683 cm-1, corresponding to the C=O stretch of bis-MPA, is no longer present and the reaction is completed. 27 The reaction was also monitored with FT Raman. The upper spectrum in figure 3.13 shows the spectrum of ER 065 with the epoxide peak at 1255 cm-1. The lower spectrum shows the modified ER 065 (HR) after a reaction time of 30 minutes with no epoxide signal. 2948 1000 ER 065 1447 3056 809 1600 1185 1031 619 1255 1726 1582 2949 Epoxide Int 1000 Reaction mixture after 30 minutes 3058 1451 1601 1184 1730 4000,0 3600 3200 2800 2400 2000 1800 1600 Raman Shift / cm-1 1031 810 1155 1400 1200 619 1000 800 600 521 400,0 Figure 3.13 FT Raman spectra of the starting resin ER 065 (upper) and the reaction mixture, 85 wt.% ER 065 and 15 wt.% bis-MPA, after a reaction time of 30 minutes (lower). Comparison of the two spectra shows the disappearance of the epoxide signal at 1255 cm-1. 3.4.3 SEC Characterization Normally, 1H NMR is a useful tool for calculating the DP for poly(ε-caprolactone). In this case however, the signals from the copolymer backbone overlaps with the signal from the methylene group next to the hydroxyl end group making accurate structure analysis difficult. On the other hand, SEC analysis supported the result of successful grafting of bis-MPA. The molecular weight increased during this first reaction from a Mw = 8200 g/mol (ER 065) to a Mw = 10 600 g/mol (HR). This increase correlates fairly well with the calculated theoretical Mw = 9800 g/mol for HR. SEC analysis also showed an increase in molecular weight, from a value of 10 600 g/mol to 33 900-38 500 g/mol for the PCL10 batches and to 55 200-62 800 g/mol for the PCL20 batches. The calculated theoretical molar mass values for PCL10 and PCL20 are 36 200 g/mol and 62 600 g/mol respectively (table 3.4). 28 Table 3.4 SEC data for the comb polymers tested, listed by synthesis batch (B = batch). In the last synthetic step, the different batches were mixed in order to reduce the number of methacrylation reactions (PCL10M, B1-B2 and PCL20M, B1-B2). APA is an acrylate functional polyacrylate derived from ER 065. Sample Mn ER 065 APA HR PCL 10 B1 PCL 10 B2 PCL 10 B3 PCL 10 B4 PCL 20 B1 PCL 20 B2 PCL 20 B3 PCL 20 B4 PCL10M B1 PCL10M B2 PCL20M B1 PCL20M B2 3 000 3 200 3 100 4 900 4 300 5 300 6 200 10 000 12 700 10 600 10 500 7 100 7 770 9 660 13 500 3 SEC 8 200 10 500 10 600 38 500 33 900 37 100 36 900 62 600 55 200 62 000 62 800 43 180 46 280 65 030 71 500 Mw Theoretical 9000 9 800 36 200 36 200 36 200 36 200 62 600 62 600 62 600 62 600 37 800 37 800 64 200 64 200 PDI 2.8 3.3 3.5 7.8 7.9 7.0 6.0 6.3 4.3 5.9 6.0 6.1 6.0 6.7 5.3 3.5 Bis-MPA Dendrimers In the early 1990’s, Hult et al. presented the first hydroxyl functional hyperbranched aliphatic polyester, as previously mentioned. This polyester was synthesized from the core moiety 2-ethyl-2-(hydroxymethyl)-1,3-propanediol (TMP) and the AB2 monomer 2,2bis(hydroxymethyl)propionic acid (bis-MPA).101 Similar hyperbranched compounds are now commercially available under the trade name Boltorn®. This work led to an attempt to synthesize the corresponding hydroxyl functional dendrimer with TMP as the core and bisMPA as the inherent structure. This attempt failed for a couple of reasons. First there were problems associated with steric hindrance in the final coupling between the dendrons (wedges) and the small core (TMP). Second there were difficulties monitoring the coupling reaction due to the absence of an UV active moiety in the core or the pre-synthesized dendrons. For this work, three sets of aliphatic polyester dendrimers based on 2,2bis(hydroxymethyl)- propionic acid (bis-MPA) were evaluated using SEC. Two of the sets had benzylidene (Bz) terminal groups and either a trimethylol propane (TMP) or triphenolic (Ar) core moiety. The last set had acetonide terminal groups and a triphenolic core moiety (figure 3.14). The synthesis of a dendrimer with a TMP core was made possible by the use of an anhydride building block. 29 O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O OO O O O O OO O O O O O O O O O O O O O O O O O OO O O O O O O O O O O O O O O O O O O O O O O O O O O O O O OO O O Bz-[G#4]-TMP O O O O O O O OO O O OO O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O Acetonide-[G#4]-Ar O O O O O O O O O O O O O O OO O O O O O O OO O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O OO O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O O OO O O O O O O O O O O O O O O O O O O O O OO O O O O O Bz-[G#4]-Ar Figure 3.14 Shown above are the 4th generation dendrimers as representatives for the three sets of dendrimers. (Bz= benzylidene terminal groups, TMP= trimethylol propane core moiety and Ar= triphenolic core moiety.) 3.5.1 SEC Characterization The SEC characterization of the dendrimers was performed using SEC3 and SECUC, previously described in section 3.2.3. The molar masses obtained with SECUC in the first analysis run (R1) of the dendrimers were close to theoretical values (table 3.5). A second run (R2) was conducted with an additional column in order to verify the reproducibility. The results from SECUC in R2 confirmed the previous R1 results. It was observed that Bz-[G#4]-TMP eluted slower than the other dendrimers of the same generation, acetonide-[G#4]-Ar and Bz-[G#4]-Ar, which eluted at the same retention volume (figure 3.15). To elucidate this further the viscosimetric radius (RV) was calculated from matrix assisted laser desorption ionization time of flight (MALDI-TOF) molecular weights and intrinsic viscosity ([η]) data from the SEC evaluation using the Einstein equivalent sphere model, 3 [η ]M Rv = 10πN A 1 3 that is based on the Stokes–Einstein relationship for the viscosity of suspended spheres. RV and hydrodynamic radius (RH) are usually identical.102,103 This agreement was observed between RV and RH values obtained by right angle laser light scattering (RALLS), with some minor discrepancies. These discrepancies were exacerbated at lower generations (RV/RH= 1.00±0.02, [G#3-5], 0.97±0.08, [G#1-2]). 30 MALDI TOF Dendrimer a g SEC a Mcalc M (g mol-1) (g mol-1) -1 PDId Mn (g mol ) SECUC b SEC3 c SECUC b R1e R2f R1e R2f R1e R2f RGg (Å) RV h (Å) Bz-[G#1]-Ar 919 917 740 730 900 1150 1.00 1.10 6.70 8.10 Bz-[G#2]-Ar 1880 1877 1670 1750 1840 2110 1.00 1.08 8.80 10.5 Bz-[G#3]-Ar 3802 3708 3830 3790 3960 3870 1.00 1.06 11.3 13.4 Bz-[G#4]-Ar 7646 7636 7640 8710 7540 7760 1.01 1.04 14.1 16.3 Bz-[G#1]-TMP 747 747 730 - 752 - 1.01 - 5.70 7.00 Bz-[G#2]-TMP 1708 1706 1630 1580 1750 1950 1.00 1.08 7.90 9.42 Bz-[G#3]-TMP 3630 3623 3680 3680 3860 4070 1.00 1.08 10.6 12.3 Bz-[G#4]-TMP 7474 7452 7350 7689 7540 7770 1.01 1.07 14.0 15.9 Bz-[G#5]-TMP 15162 15099 14690 16000 14550 14920 1.02 1.04 17.1 20.1 Acetonide-[G#1]-Ar 774 - - 834 - 1100 - 1.08 7.40 7.40 Acetonide-[G#2]-Ar 1592 1588 1780 1850 1600 2080 1.00 1.07 7.70 9.78 Acetonide-[G#3]-Ar 3226 3221 3400 3730 3230 3920 1.00 1.03 10.4 12.6 Acetonide-[G#4]-Ar 6493 6486 7340 7300 5710 7080 1.01 1.01 13.3 16.2 + b c d e f Measured M-Ag ; Universal calibration method; Tripel detection calibration method; Polydisperisty index; single separation column; two separation columns; radius of gyration; h Viscosimetric radius. Table 3.5 MALDI-TOF and SEC data for dendrimers consisting of different: generations, end-groups and core molecules. 31 110 Bz-[G#4]-TMP ___ Bz-[G#4]-Ar Acetonide-[G#4]-Ar U 87 Relative response _______ __ ____ ___ × 64 41 18 -5 8.0 8.5 8.9 9.3 9.8 10.2 Elution volume (mL) Figure 3.15 The retention volume for all 4th generation dendrimers: of Bz-[G#4]TMP, Bz-[G#4]-Ar and Ac-[G#4]-Ar. The plot of RV against M (figure 3.16) shows the size of the three sets of dendrimers and an additional set of acetate-[G]-Ar dendrimers. The acetate-[G]-Ar were originally synthesized by Hult et al. and their self diffusion constant was studied utilizing pulsed field-gradient spin-echo (PGSE)-1H NMR in CDCl3.73 The published RV values of acetate-[G]-Ar were close to the RV data obtained for the dendrimers in this study. However, direct comparison of the results is not possible as the current work utilized THF as the solvent and it may have affected the RV. The terminal groups, acetonide and Bz appear to have no significant impact on the RV of the studied generations. However, Bz-[G]-TMP exhibits a slightly smaller size and this is related to the smaller core molecule. The ratio RG/RV = 3 / 5 ≈ 0.77 for a sphere of uniform density. There have been a number of publications utilizing this ratio for dendrimer analysis, especially for poly(propylenimine) (PPI) dendrimers, using low angle light scattering.104,105,106 For PPI dendrimers, the RG/RV ratio was to found to exhibit a semi quantitative relationship.106 It was also determined that the solvent may have a large impact on the measurement of RG and RV. 32 20 V R (Å) Bz-[G]-Ar Bz-[G]-TMP Acetonide-[G]-Ar Acetate-[G]-Ar 10 9 8 7 1000 4 -1 Molecular weight (g mol ) 10 Figure 3.16 RV as a function of molecular weight. The acetate-[G]-Ar data determined by PGSE-1H NMR in CDCl3 are from a previous study by Hult et al.73 SEC3 evaluation also yielded the radius of gyration (RG) of the dendrimers calculated using the Flory-Fox107 and Ptitsyn-Eisner equation:108 1 1 1 2 [η ]M 3 RG = 6 F ( ) where F = 2.86 ⋅ 10 21 1 − 2.63e + 2.68e 2 , e = (2α − 1) / 3 , and α is the exponent of the Mark-Houwink equation: [η] = kM α . The data obtained suggests spheres of uniform density, values fairly close to 0.77, for all of the dendrimers except acetonide-[G#1]Ar. However, in view of the use of α from the Mark-Houwink equation to obtain the RG and the fact that determining α accurately requires a polydisperse sample, the RG data is to be regarded as uncertain. In addition, the Flory-Fox and Ptitsyn-Eisner equation is derived for linear and flexible polymers. The molecular weights obtained with light scattering were, in general, close to the theoretical and MALDI-TOF values. Some of the deviation of the SEC values from the theoretical values can be explained by a combination of factors, such as the small amount of compounds available for analysis and the low concentrations used (4-6 mg ml-1). Acetonide-[G]-Ar exhibited a poor signal to noise ratio due to a low refractive index increment, also contributing to experimental error. 33 For polymers in general, there is a linear logarithmic relationship between [η] and molecular weight, but for dendrimers the viscosity starts to decline at a certain generation due to conformational change to a globular structure.58 This reduction in [η] was observed for Bz-[G]-Ar and Bz-[G]-TMP (figure 3.17) of the 4th and 5th generation, respectively. However, acetonide-[G]-Ar did not display this characteristic reduction of [η], at least not below the 5th generation, whereas the [η] of Bz-[G]-Ar was at its maximum at the 3rd generation. Theoretical calculations have predicted increased crowding at the surface as the number of generations increase.109 For acetonide-[G]-Ar, this crowding might occur at a higher generation due to the less bulky terminal acetonide groups as compared to the bulky benzylidene groups found in Bz-[G]-Ar. [η] (dL/g) 0.04 0.03 Bz-[G]-Ar Bz-[G]-TMP Acetonide-[G]-Ar 1000 10 4 -1 Molecular weight (g mol ) Figure 3.17 Intrinsic viscosity ([η]) as a function of molecular weight. 34 4. Rheological Characterization Rheological behavior is important since it controls the deformation and flow properties of polymers. In order to evaluate the flow properties of branched semicrystalline resins, a number of rheological experiments were preformed. Zero shear viscosity measurements were performed to evaluate the flow properties at very low shear rates such as those present at coating leveling. UV-curing behavior was also studied in order to investigate curing performance. Lastly dynamic viscosity measurements were made to study the relationship of complex viscosity and temperature, an important feature of semi-crystalline, solid coating materials. 4.1 Zero Shear Viscosity of Star-Branched Poly(ε-caprolactone)’s The viscoelastic properties of polymers are strongly influenced by chain entanglement.110 Chain entanglement occurs naturally in a melt when critical molecular weight, Mc, is reached. Architecture also has a pronounced effect on the viscosity of a polymer (figure 4.1). A linear PCL was synthesized and analyzed for comparison. The linear PCL was found to follow the power law, using the molecular weight obtained from SECUC, given by the expressions: η0 = 4.65×10-8 M1.99 M<Mc, Mc=7500 g mol-1 η0 = 2.80×10-13 M3.34 M>Mc The deviation from η0 ∝ M for M<Mc can be attributed the lack of correction made for the change in the monomeric friction coefficient.55,57 Correction of the curve is not within the scope of this study. The Mc value is equivalent to about 450 atoms in the main chain, which is in the range expected for a highly flexible chain. 55,57 This type of measurements are normally performed on polymers synthesized by anionic polymerization, which results in polymers with narrow PDI. 35 1000 10 0 η (Pa s) 100 Linear PCL, Mw<Mc Linear PCL, Mw>Mc Dendron-PCL Dendrimer-PCL Boltorn-PCL 1 0.1 1000 10 4 5 10 6 10 -1 M (g mol ) w Figure 4.1 Zero shear viscosity as a function of Mw obtained from SECUC. As mentioned previously, the zero shear viscosity (η0) increases exponentially with molecular weight for star-branched polymers.67 The viscosity of a star polymer with 4 or more arms is dependent on the arm length or degree of polymerization (DP) while independent of the number of arms and the total molecular weight.68,111 This can be seen for star-branched polymers when plotting viscosity as a function of arm molecular weight (figure 4.2). Arm molecular weight (Ma) was calculated from Mw by subtracting Mcore and then dividing by the theoretical number of arms. In general, data scatter can be explained by the degree of functionalization at low M and by polydispersity. In addition, there is some uncertainty regarding the number of hydroxyl groups on Boltorn since its structure is less exact than the dendrimer. 36 1000 Dendron-PCL Dendrimer-PCL Boltorn-PCL 0 η (Pa s) 100 10 1 100 4 1000 10 5 10 -1 M (g mol ) a Figure 4.2 Viscosity as a function as Ma obtained from SEC. Measurements were conducted at 90°C so that the viscosity values of all of the samples were in the measurable range of the equipment. 4.2 UV-Curing Rheological Behavior of Star-Branched Poly(ε-caprolactone)’s During resin cross-linking, the system reaches the gel point at which time the reactive system loses the ability to flow. This is one of the most important kinetic characteristics of cure. According to Flory, the gel point is characterized by the appearance of a macromolecule with an infinitely large molecular weight.111 Some fast curing systems reach 50% conversion in 0.3 s.112 Rapid conversion such as this makes it difficult to use classical methods and equipment to monitor the reaction. Månson et al. have developed a new method of measuring the viscoelastic behavior of fast curing systems.113 Using a commercial rheometer coupled to an UV-light source, the viscoelastic behavior can be measured in ultra fast reacting systems. This novel set-up is particularly suited for determining gel point, vitrification, if it occurs, and modulus evolution of fast UV-curing systems. Rheological behavior during UV-curing was measured on four different samples of Boltorn-PCL. The molecular weight of the Boltorn-PCL star polymers ranged from 77 000 to 193 000 g mol-1 and the distribution ranged from 1.3 to 1.8 (table 4.1). As previously mentioned, the gel point is the most important factor influencing the processing of thermosets since flow becomes restricted at this point. At the gel point, the material transitions from a liquid to a solid state and thereafter deformation may cause damage to the formed network. 37 Table 4.1 Data collected on Boltorn-PCL material used in the study of the UV-curing rheological behavior. The SEC data was obtained using conventional calibration. Sample Boltorn-PCL DP, aim DP, NMR Mw, NMR (g mol-1) Mw, SEC (g mol-1) Mn/Mw DP20 DP30 DP40 20 30 40 50 20 30 38 52 76 600 113 000 142 200 193 300 70 700 96 100 105 400 153 000 1.25 1.25 1.39 1.78 DP50 According to Winter and Chambon114,115, the gel point can be determined from dynamic mechanical measurements of the frequency dependence of the loss tangent (tan δ). The gel point is defined as the point at which tan δ is independent of the frequency, i.e. at the intersection of tan δ at different frequencies. Figure 4.3 is a plot of tan δ for the different frequencies of Boltorn-PCL DP30. Although a trend in gel times was recorded for the resins, no clear intersections could be observed. It was therefore impossible to draw any conclusions from this data concerning the gel point. The ambiguity was probably due to a slight mistiming when superimposing the tan δ curves from the four different frequencies, an occurrence that becomes more evident when dealing with gel times on the order of 0.4 seconds. Normally, this problem is solved with simultaneous multi-wave measurements. However, the sampling rate on normal equipment is approximately every 8 seconds, far too slow for the system investigated here. 18 40 Hz 16 14 60 Hz Tan δ 12 10 80 Hz 8 99 Hz 6 4 2 0 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5 Time (s) Figure 4.3 Tan δ of Boltorn-PCL DP30 at 40, 60, 80 and 99 rad s-1. UV irradiation commenced at t=2 s. 38 To overcome this sampling limitation, a data reduction program developed by Månson et al. allowing a sampling rate of every 0.01 second was used.116 This procedure consisted of applying arbitrary wave shaped, strain controlled oscillations at four different frequencies on four distinct samples, extracting the tan δ curves and superposing them to seek the crossover. However, since this method ultimately yielded ambiguous results, it was preferred to use the crossover point of the storage modulus, G’, and the loss modulus, G’’, to determine the gel point.117,118 Although this method of identifying the gel point is common industrial practice, it is not supported by theoretical arguments except for in the case of one class of polymers119 Those which exhibit power law relaxation G(t)~t-1/2 when reaching the gel point. Examples are stoichiometrically balanced network polymers and network polymers with excess cross-linker, but only at temperatures high above Tg. When the crossing of G’ and G’’ was applied to the investigated system, the gel point was reached within seconds and showed no clear frequency dependence (figure 4.4). The time to reach gel point increased linearly with DP. This relationship follows kinetic theory, since the concentration of methacrylate end groups decreases with increasing Mw. 4.5 4 Time at tan δ =1 (s) 3.5 3 2.5 2 1.5 1 0.5 0 0 10 20 30 40 50 60 Degree of Polymerization Figure 4.4 Time to G’ and G’’ crossover for 40 (+), 60 (Ο), 80 (−) and 99 (U) rad s-1. UV irradiation commenced at t=2 s. In order to obtain clear experimental results for the initial part of the reaction, large strain was used due to the low viscosity of the resins. Figure 4.5 shows a run that was used to obtain the G’ G’’ crossover point for Boltorn-PCL, DP50. However, the higher strain caused either the samples to fracture or the apparatus to overload, as the modulus increased, thus full cure was not achieved. Hence, the strain was reduced in order to measure the evolution of G’ and G’’ to full cure (figure 4.6). Complete leveling off of the modulus required 20 to 30 s. A drop in G’’ was observed shortly after crossing G’ to which there was no apparent explanation. 39 5 G' G'' 10000 4 1000 3 100 2 tan δ 10 tan δ G', G'' (Pa) 100000 1 1 0 0 1 2 3 4 5 6 7 Time (s) Figure 4.5 G’ and G’’ for Boltorn-PCL, DP50, measured at 40 rad s-1. UV irradiation commenced at t = 2 s. 10000000 G', DP30 G', DP20 G', DP40 1000000 G', G'' (Pa) 100000 G', DP50 G'', DP30 G'', DP20 G'', DP40 G'', DP50 10000 1000 100 10 1 0 10 20 30 40 50 60 70 Time (s) Figure 4.6 Evolution of G’ and G’’ to full cure. Since no change in Tg occurred during cross-linking, the cured material was rubbery at the curing temperature, 75°C. The modulus at the rubber plateau decreases with increasing DP (figure 4.7) since the distance between cross-links increases. Upon 40 cooling, the cross-linked material crystallized. Upon cooling, the cross-linked material crystallizes to a varying extent depending on the DP, with the degree of crystallization increases with increasing DP (table 2). Calculations of degree of crystallization were carried out using 166.5 J g-1 as the heat of fusion for a 100% crystalline material.120 There is also an increase of the melting temperature with increasing molecular weight. 1.8 1.6 1.4 G' (MPa) 1.2 1 0.8 0.6 0.4 0.2 0 0 10 20 30 40 50 60 Degree of Polymerization Figure 4.7 G’ as a function of DP after full cure at 75°C. Table 4.2 DSC data of the cross-linked films. Sample Boltorn-PCL20 Boltorn-PCL30 Boltorn-PCL40 Boltorn-PCL50 Degree of crystallisation (%) 29 41 42 50 Onset of melting (°C) 34.3 41.3 47.9 50.2 Peak of melting (°C) 45.3 51.7 53.6 58.6 41 4.3 Dynamic Viscosity from Solid to Molten State An important feature of the semi-crystalline resins is their fast transition from the solid to the molten state. This characteristic will permit the use of lower curing temperatures since the modulus of the resin is maintained until the melting temperature (Tm) is reached. Figure 4.8 depicts the complex viscosity (η*) as a function of temperature of a number of different synthesized resins. The measurement of η* during the melting transition of semi-crystalline resins shows a rapid decrease in viscosity over a narrow temperature range, as compared to the slow softening of the amorphous acrylate functional polyacrylate resin (APA). This rapid reduction in viscosity of semicrystalline resins gives them an advantage when compared to conventional amorphous resins with thermal initiators, which soften slowly from Tg until the point where the cross-linking reaction starts to increase the viscosity. For example, the semicrystalline PNPC displays a melting temperature almost ideal for a low temperature curing powder coating resin, just below 100°C. APA Comb PCL DP10 Comb PCL DP20 Boltorn-PCL DP10 Boltorn-PCL DP20 Di-TMP-PNPC DP8 8 10 6 η* (Pa s) 10 4 10 100 1 0 50 Temperature (°C) 100 150 Figure 4.8 Dynamic viscosity as a function of temperature for 4 types of different resins. 42 4.3.1 Comb Poly(ε-caprolactone)’s and blends To further widen the scope of this work, blends were prepared of the amorphous resin APA and the comb-PCL’s. 9 10 APA APA:Comb-PCLM DP20, 7:3 APA:Comb-PCLM DP10, 3:2 APA:Comb-PCLM DP20, 1:1 Comb-PCLM DP20 Comb-PCLM DP10 8 10 7 10 6 η* (Pa s) 10 5 10 4 10 1000 100 10 0 50 100 150 Temperature (°C) Figure 4.9 Complex viscosity as function of temperature for some of the different resins and resin blends. The measurement of η* of the blends revealed a rheological behavior which falls between those of its individual components (figure 4.9). The complex viscosity for PCL10M started to decrease before that of PCL20M, which is consistent with the Tm results from the calorimetric data (table 4.3). The melting points of the comb-PCL’s are lower than that of linear PCL, which exhibits a Tm of around 65°C. The 1:1 blends exhibit some crystalline behavior while the 3:2 and 7:3 blends behave as if fully amorphous. The samples containing crystalline resin were all cooled the same way, from 140 to –10°C, before the measurements began. This cooling did not allow enough time for these PCL in the blends to crystallize to its full extent and it is therefore likely that the resins would display behavior close to that seen with 1:1 blends. The η* at higher temperatures is also lower for the blends, facilitating leveling and resulting in smoother films. 43 Table 4.3 DSC-data of the synthesized semi-crystalline resins. a 44 Sample Tg Tm, peak a DCb % a ER 065 PCL10 B2 PCL10 B2 PCL20 B2 PCL20 B2 50c -54 -55 -54 -55 36 38 47 47 29 34 35 35 Second heating, bDegree of crystallinity, c BASF AG 5. Film Characterization 5.1 Mechanical Properties of Star-Branched Poly(ε-caprolactone) Film properties were evaluated after cross-linking. The polyester and the photoinitiator Irgacure 184™ (1% by wt.) were added to just enough butyl acetate to dissolve the polymer. The mixture was then applied with a 700 µm applicator onto a glass plate. After evaporation of solvent at RT, the film was melted at 70 °C and then immediately UV-cured with 5 subsequent passes under the UV-lamp, giving a total dose of 500 mJ cm-2. The dynamic mechanical properties of six cross-linked Boltorn-PCL films were examined at temperatures between -70 and 100°C (table 5.1). The average film thickness varied between 60-130 µm. All samples had an onset of Tg close to –50°C which was as expected for CL based polymers. The dynamic mechanical thermal analysis (DMTA) data shows that the cross-linking of the films reduced the possibility for the PCL-chains to crystallize when the films were cooled. The resins with short PCL-chains, DP 8 or less, did not crystallize at all in the cross-linked state, while resins having longer PCL-chains, crystallized to some extent. In previous work, calorimetric data of similar films have shown that the degree of crystallization in the cross-linked films of long-chained resins is approximately 50% as compared to the uncured resin.121 Table 5.1 DMTA of cross-linked Boltorn PCL films, where E is the Young’s modulus. Boltorn-PCL E (MPa) E (MPa) E (MPa) (DPNMR) (t=-55 °C) (t=23°C) (Rubber-plateau) 5 8 20 30 38 52 1770 1600 1350 380 440 1410 15 16 94 45 79 250 15 16 2.3 0.9 ~1 ~1 The effect of crystallization in the cured film is clearly seen in figure 5.1, where the semi-crystalline film maintains a higher modulus above Tg as compared to the amorphous film. Above the melting point, the modulus for crystalline resins drops to a level lower than that for amorphous resins since the crystalline resins have a lower cross-link density. The results show that the structure of a resin has a pronounced effect on the final film properties and, thus, by altering the structure a resin can be tailored for a specific application. 45 Young's modulus (MPa) 10000 1000 Semi-crystalline 100 Amorphous 10 1 -80 -60 -40 -20 0 20 40 60 80 100 120 Temperature (°C) Figure 5.1 Young’s modulus as a function of temperature. The semi-crystalline and the amorphous films have DP’s of 52 and 5, respectively. 5.2 Properties of Comb Poly(ε-caprolactone) Films The study of comb polymers was made to investigate the overall effect on film properties of varying the graft length. In addition, blends of amorphous and semicrystalline resins were evaluated with respect to length of the grafts and blend ratio. To give some insight into these relationships, an epoxy functional acrylic resin (ER 065) was modified into a semi-crystalline thermosetting resin (section 3.4). 5.2.1 Powder and Film Preparation All resins were melt-mixed with photoinitiator (Irgacure 2959, 2 wt.%). Pulverization was performed using dry ice since the resins were slightly tacky at room temperature. The resulting powder was sifted through a 150 µm sieve and applied to a steel substrate with an electrostatic spray gun. The combination of the low Tm and low Tg of poly(ε-caprolactone) made grinding, sieving and spraying tricky and storing at room temperature impossible. The powders were fused for 15 minutes at 140°C. This temperature was chosen so that all the films and resins, amorphous, semi-crystalline and mixtures thereof, would undergo the same fusing conditions. Another set of films was fused in an IR oven at 140°C or 160°C for two minutes. However, the 2 minute exposure was not long enough to produce an even surface, a requirement for the mechanical testing. The curing was initially performed using two different pieces of equipment, a UV-Minicure with a single high-pressure mercury lamp and a high power irradiator, HL-60-3X1, using three lamps, two high-pressure mercury lamps and a gallium doped mercury lamp. 46 Table 5.2 Cure conditions and mechanical properties of the cured films. All films were fused in a convection oven at 140°C for 15 minutes. No orange peel texture was observed for any of the films and the gloss was poor for all films. The cross-cut range from Gt 0-Gt 5 where Gt 0 is the best. All films were prepared from resins from the second batch Sample Curing Comb-PCL10M Comb-PCL10M Comb-PCL20M Comb-PCL20M UV Minicure HL-60-3X1 UV Minicure HL-60-3X1 Erichsen test [mm] 8.4 8.6 9.4 8.8 Diameter at break [mm] 4 6 2 3 Cross-cut test Gt 5 Gt 5 Gt 5 Gt 4 The films cured with higher irradiation intensity, HL-60-3X1, were slightly more brittle, as exhibited by the Erichsen and bending test results (table 5.2). Higher irradiation intensity results in a greater number of radicals, which in turn leads to a shorter kinetic chain length and decreased cross-link density. Films cured using the UV-Minicure were tacky, a sign of oxygen inhibition. The high intensity system produced films without a tacky surface and was therefore used to cure all films for which film properties were to be evaluated. It is also evident from the Erichsen and bending tests, tables 5.2 and 5.3, that PCL20 exhibits a greater flexibility, as expected, than the PCL10 resin due to the lower cross-link density of PCL20. 5.2.2 Film Properties Different ratios of Comb-PCL10M:APA and of Comb-PCL20M:APA were evaluated to identify which blends showed the best characteristics (table 5.3). More blends were made with PCL10 as it was less tacky, which made processing easier. The Comb-PCL10M:APA 4:6 blend exhibited the best overall properties. The results show that it is possible to use the highly branched structures to modify a system and improve its properties. The fact that APA has acrylate functionality and the semicrystalline resin has methacrylate end groups, will give different polymerization rates. How this affects the system is not known. 47 Table 5.3 Film properties of the evaluated films. Sample, Blend ratio Erichsen test[mm] Diameter of break [mm] Cross-cut test Gloss Surface APA 0.3 - Gt 5 Good Orange peel Comb-PCLM 10:APA, 3:7 4.3 - Gt 3 Fair Smooth CombPCLM 20:APA, 3:7 4.4 - Gt 3 Fair Smooth CombPCLM 10:APA, 4:6 5.3 8 Gt 1 Fair Smooth CombPCLM 10:APA, 1:1 7.3 6 Gt 4 Fair Smooth CombPCLM 20:APA, 1:1 5.8 6 Gt 4 Fair Smooth CombPCLM 10 8.6 6 Gt 5 Poor Smooth CombPCLM 20M 8.8 3 Gt 4 Poor Smooth One factor to note with these resins is the fact that even a high molecular weight semi-crystalline resin will help the leveling of the film. The APA resin by itself is not able to produce a film without orange peel while the PCL20M resin and blends thereof with a molecular weight of about 60 000 g/mol produce smooth films. Addition of a high molecular weight resin can also reduce the shrinkage upon cure, which in turn will reduce internal stress buildup. An important point to keep in mind is that there is a conflict between cross-linking density and crystallinity. The grafts have to be long enough to ensure crystallinity and yet short enough not to crystallize after cross-linking. The cross-link density of this type of resin is low, which makes the final films flexible. On the other hand, this is not necessarily a problem since the substrates for low temperature curing, paper, plastic materials and wood, are inherently flexible. The problems associated with use of a pure semi-crystalline resin, the process problems and poor mechanical properties, might be avoided by using grafts of a crystalline polymer with the right combination of Tg and Tm, preferably in the range of 30-40°C and 80-100°C, respectively. 48 6. Conclusions The concept of aUV-curable branched semi-crystalline thermoset resin was evaluated. The poly(ε-caprolactone) system confirmed the anticipated advantages, include low zero shear viscosity, rapid reduction of viscosity at the melting temperature, and fast curing. It was shown that the molecular weight can be increased about one order of magnitude using a star-branched polyester with aproximately30 arms over that of a linear polyester while maintaining the zero shear viscosity. The high molecular weight in the range of interest, up to 10-20 Pa s of zero shear viscosity, can reduce or eliminate unwanted penetration of a porous substrate. In addition, the semi-crystalline resins exhibit a fast decrease in viscosity around the melting temperature as compared with the slow softening of an amorphous resin. After leveling, UV initiated cure is completed in a matter of seconds. Even though the time to gel increased linearly with increasing molecular weight when using the G’ and G’’ crossover as the gel point, time to gel was less than 2 s. Dynamic mechanical data show that the rubber plateau modulus decreases with increasing length of the poly(ε-caprolactone) grafts. An important point to keep in mind is that there is a conflict between cross-linking density and crystallinity. The grafts have to be long enough to ensure crystallinity and yet short enough not to crystallize after cross-linking. The low cross-link density and glass transition temperature makes the star-branched poly(ε-caprolactone) films flexible and soft. In the cured films the degree of crystallization depends on the length of the PCL-grafts. Post cure crystallization can be avoided by using short grafts, around DP=10, for star PCL’s. The dynamic viscosity measurements of the melting transition clearly showed the advantage of a semi-crystalline system, specifically the rapid decrease in viscosity at Tm. Thermosetting comb-polymers with semi-crystalline grafts were also synthesized in a straightforward manner requiring only three steps from a starting epoxide functional amorphous resin. The synthesis allowed good control of the structure and molecular weight. The resulting semi-crystalline resins displayed relatively high crystallinity and a considerably depressed melting point compared to linear poly(εcaprolactone). The low melt viscosity resulted in smooth films. The flexibility of the films containing a blend of semi-crystalline and amorphous resin was also improved compared to the films of pure amorphous resin. This was due to a decrease in crosslink density and the low Tg of the poly(ε-caprolactone) grafts. The main drawback was the poor storage stability of the semi-crystalline powders and the blends. In addition, the mechanical properties of the model poly(ε-caprolactone) systems are not ideal. However, the concept provides advantages, such as low viscosity, high molecular weight, improved storage stability, low toxicity and absence of a low molecular weight binder, compared to conventional powder coating systems. The branched poly(neopentylene carbonate) on the other hand displays a Tm around 100°C and a Tg around 20-30°C which is more suitable for a low temperature curing powder coating. The dynamic viscosity measurements also showed that the resins maintained a high ‘viscosity’ until close to melting. This should allow for good storage stability and reasonable mechanical properties. However, the control of the polymerization was low; as a consequence the yield was also low. SEC molecular weight data collected on the series of dendrimers using SECUC and SEC3 were close to the theoretical and MALDI-TOF values. Calculations of the viscosimetric radii showed a difference in size for Bz-[G]-TMP compared to the 49 acetonide/Bz-[G]-Ar dendrimers. This difference is associated to the difference in size of the core molecule. It was also showed that the terminal unit had no effect on the viscosimetric radius. The ratio Rg/RV suggests that that the dendrimers behave as uniform-density spheres. The intrinsic viscosity of acetonide-[G]-Ar revealed a delayed viscosity maximum compared to Bz-[G]-Ar, which might be explained by its less congested surface. 50 7. Suggestions of further work For the possible use of highly branched semi-crystalline resins in powder coating application very little work has been carried out, to our knowledge. Since there are a number of advantages a more thorough investigation of this concept is warranted using other monomers to produce systems with better overall properties. The branched poly(neopentylene carbonate) displays promising powder coating properties which warrants a further investigation into their cross-linked film properties. In addition, the highly crystalline poly(ω-pentadecalactone) with a Tm of around 90°C might be a suitable candidate for coating application, however the Tg is very low. There are also a number of different dendritic initiators available. A hyperbranched hydroxyl functional polyether might provide an increased outdoor stability. This particular core is readily available within the group. In the near future a hyperbranched polycarbonate might be available for evaluation. Another possible study of these polymers is as rheological additives in established coating systems. 51 Acknowledgements I would like to express my gratitude to my supervisor Professor Anders Hult for accepting me as his graduate student, providing guidance, sharing his extensive knowledge and making the group a great place to work and develop. I would also like to thank the senior members of the Hult group, my co-supervisor, Associate Professor Eva Malmström and Associate Professor Mats Johansson; Eva, for always being enthusiastic, and for her insightful help, without her this work would have been much harder; Mats for his support, interesting discussions and input to my work. Financial support provided by Perstorp AB and AB Wilhelm Becker is gratefully acknowledged. Professor Jan-Anders Månson and Marc Doyle, both co-authors, are gratefully acknowledged for making my visit to Lausanne productive and enjoyable. I am indebted to Dr. Christian Kugge at The Institute for Surface Chemistry, Thomas Larsson and especially Björn Atthoff in the Hillborn group at Uppsala University, Department of Material Chemistry, for providing access to and guidance in using their rheometer. I would like to thank Professors Ann-Christine Albertsson, Bengt Stenberg and Sigbritt Karlsson for organizing and leading the Department of Polymer Technology. Especially, Ulf Gedde and Mikael Hedenqvist are acknowledged for there the interesting discussions The members of Professor Hult’s group, both past and present; Curzio, the Italian Chorizio, Johan, I still haven’t seen you play with the band, Henrik (I), the king of dendrimers and cheap shots, Anna, Daniel, Cecilia, Geraldine, Linda S., Thierry, Phil, Claire, Helene, Linda, my favorite diploma worker-good luck with your PhD, Emma and Josefina are thanked, if not their help, for the many fun times spent together. Some people in the group require some special recognition: Andreas Krupicka for always being a good sport and friend, who also engaged me in interesting discussions regarding everything from polymer mechanics to the secret of a really good cup of coffee. Peter Löwenhielm for always trying my patience and for his ability to create complete disorder in the whole lab, single-handedly. During the years there have also been interesting collaborations that made this thesis possible. You’re the man! The “time-martyr” of the group, Michael “I work better at night (zzzz…)” Malkoch, sucking the life-force out of the group in the last days of his thesis writing, is thanked for making the world and the group a better place. See ya in California! Super host Robert “I know everything” Vestberg for arranging great parties, frequently; making sure everyone gets their ration of “Labimner”. Andreas “I know the rest” Nyström for his extensive knowledge in most matters and his first-rate proofing. All my friends in the department, former and present, are also thanked for making it a great place to work. Special thanks go to Eugenia, Micke “The party never ends” Krook, Ana, the excellent hostess of many gatherings, Kamyar with whom I shared an 52 office and Guillaume with whom I never want to share an office, and Richard “The Nano Particle” Olsson for the interesting conversations about everything from science to heavy metal. I would also like to thank the administrative personnel of the department, especially Inger Lord and Margareta Andersson for their valuable assistance with all administrative matters. I would like to give special thanks to Dr. Mikael Trollsås and Dr. James L. Hedrick for accepting me as a diploma worker and later as an intern at IBM/CPIMA and for introducing me to the world of hands-on polymer chemistry. Micke also introduced me to the pleasure of wine (and the questionable one of grappa); I hope to see you on the tennis court again. The time spent in California was fun and instructive and not only did it result in me continuing my education for a PhD. During my time in the California I meet the love of my life, Laura my wife, who has been supporting me in all aspects of life including but also in my research with discussions and the excellent proofing of all my writing, that sometimes makes as little sense as me…. Last but not the least; I would like to express my sincere thanks to my parents, Annika and Ingemar for all the support and encouragement over the years as a student to reach this goal. I also want to thank my siblings Lisa and Anders, and all my relatives all over the world for their support and encouragement of me becoming a plastic doctor. 53 References 1 J.D. Crowley, G.S. Teague, L.G. Curtis, R.G. Foulk, F.M. Ball Journal of Paint Technology, 44, 56, 1972. 2 S.E. Orchard Appl. Sci. Res., A11, 451, (1962). 3 M. Osterhold, F. Niggemann Progress in Organic Coatings, 33, 55, 1998. 4 T.A. Misev Powder Coating – Chemistry and Technology, John Wiley & Sons, (1991). 5 Z.W. Wicks, JR, F.N. Jones, S P. Pappas Organic Coatings - Science and Technology, 2nd ed. Wiley-Interscience, (1999). 6 L. Kapilow, R. Samuel Journal of Coatings technology, 59, 39, (1987). 7 V.G. Nix, J.S Dodge Journal of Paint Technology, 45, 59, (1973). 8 S. Udding-Louwrier, R.A. Baijards, Sjord de Jong Journal of Coatings technology, 72, 71, (2000). 9 A. Tinnemans, A. Roeschers Progress in Organic Coatings, 40, 191, (2000). 10 K.D. Weiss Progress in Polymer Science, 22, 203, (1997). 11 R.J. Young, P.P. Ang Interfacial Phenomena in Composites Materials’ 291, Butterworth-Heinemann Ltd, Oxford, (1991). 12 C. Zune, K. Buysens European Coatings Journal, 5, 18, (2000). 13 S. Laihonen Self Diffusion in an Organic Powder Coating, Master Thesis, Dept. Polym.Techn., Royal Institute of Technology, Stockholm, Sweden, (1991). 14 L. Moens, J-M. Loutz, D. Maetens, P. Loosen, M Van Kerkhove Patent US5639560. 15 J.G. Hillborn, S.E. Jönsson, P.M.E. Stödeman, O.S.G. Skolling Waterborne High Solids and Powder Coating Symposium, New Orleans, LA, februari, p. 54, (1991). 16 T.A Misev, R. van der Linde Progress in Organic Coatings, 34, 160, (1998). 17 D.A. Tomalia, H. Baker, J.R. Dewald, M. Hall, G. Kallos, S. Martin, J. Roeck, P. Smith Polymer Journal (Tokyo), 17, 117, (1985). 18 D.A Tomalia,. A.M. Naylor, W.A Goddard Angewandte Chemie, International Edition, 29,138, (1990). 19 J.M.J. Fréchet Science, 263, 1710, (1994). 20 G.R. Newkome, Z. Yao, G.R. Baker, V.K. Gupta Journal of Organic Chemistry, 50, 2003, (1985). 21 C.J. Hawker, J.M.J. Fréchet Journal of the American Chemical Society, 112, 7368, (1990). 22 H. Ihre, O. L. Padilla, J.M.J. Fréchet Journal of the American Chemical Society, 123, 5908, (2001). 23 Y.H. Kim, O.W. Webster Polym. Prepr., 29, 310, (1988). 24 P.J. Flory Journal of the American Chemical Society, 74, 2718, (1952). 25 C.J. Hawker, R. Lee, J.M.J. Fréchet Journal of the American Chemical Society, 113, 4583, (1991). 26 C.J. Hawker, E.E. Malmstrom, C.W. Frank, J.P Kampf, C. Mio, J. Prausnitz Polymeric Materials Science and Engineering, 77, 61, (1997). 27 E. Malmström, A. Hult Macromolecules, 29, 1222, (1996). 28 E. Malmström, M. Johansson, A. Hult Macromolecules, 28, 1698(1995). 29 B. I. Voit. 35th IUPAC Int. Symp. on Macromolecules, Akron, Ohio, USA, (1994). 30 J.E.L. Roovers Dendrimers and Other Dendritic Polymers, Ed. J.M.J. Fréchet, D.A. Tomalia, Wiley N.Y. (2001). 31 J.E.L. Roovers, S. Bywater Macromolecules, 5, 384, (1972). 54 32 J-S.Wang, D. Greszta, K. Matyjaszewski Polymeric Materials Science and Engineering, 73, 416, (1995). 33 J. Xia, X. Zhang,K. Matyjaszewski Macromolecules, 32, 4482, (1999). 34 C.J. Hawker Angewandte Chemie, International Edition, 34, 1456, (1995). 35 J. L. Hedrick, M. Trollsås, C. J. Hawker, B. Atthoff, H. Claesson, A. Heise, R. D. Miller, D. Mecerreyes, R. Jerome, Ph. Dubois Macromolecules, 31, 8691, (1998). 36 H. Beerens, F. Verpoort, L. Verdonck Journal of Molecular Catalysis A: Chemical, 151, 279, (2000). 37 M. Stenzel-Rosenbaum, T.P. Davis, V. Chen, A.G. Fane Journal of Polymer Science, Part A: Polymer Chemistry, 39(16), 2777, (2001). 38 C.S. Gudipati, E.E Remsen, K.L. Wooley Polymeric Materials Science and Engineering, 88, 610, (2003). 39 F. Wang, R.D. Rauh Patent US 6025462, (2000). 40 J. Huybrechts, K. Dusek Surface Coatings International, 81(3), 117, (1998). 41 L. Phan, A. Mukherjee, R. Farwaha, J.S. Thomaides Eur. Pat. Appl. EP1219650, (2002). 42 P.K. Agarwal, H-C.Wang, Y.F.Wang, J.M.J. Fréchet, S.A. Haque Patent US6228978, (2001). 43 S.L Bennett, Y. Jiang, E.A. Gruskin, K.M. Connolly Patent US5578662, (1996) 44 T.A. Orofino Polymer, 3, 295 and 305, (1968). 45 H.A.J. Battaerd, G.W. Tregear Graft Copolymers New York: Wiley/Interscience, (1967). 46 P. Dreyfuss Encyclopedia of Polymer Science and Engineering 2nd ed. Vol.7 New York: Wiley/Interscience, (1988). 47 K.J. Ivin, T. Saegusa Ring-opening polymerization Vol.1 Ed. K.J. Ivin, T. Saegusa Elsevier, NY, (1984). 48 M.H. Hartmann Biopolymers from Renewable Resources Ed. D.L. Kaplan, Springer, Berlin, (1998). 49 S. Penczek, A. Duda, A.Kowalski, J. Libiszowski, K. Majerska, T. Biela Macromolecular Symposia, 157, 61, (2000). 50 H.R. Kricheldorf, I. Kreiser-Saunders, C. Boettcher Polymer, 36, 1253, (1995). 51 A. Kowalski, A. Duda, S. Penczek Macromolecular Rapid Communications, 19, 567, (1998). 52 T. Endo, Y. Shibasaki, F. Sanda Journal of Polymer Science, 40, 2190, (2002). 53 C.J. Hawker Dendrimers and Other Dendritic Polymers, Ed. J.M.J. Fréchet, D.A. Tomalia, Wiley N.Y., (2001). 54 S. Penczek Makroloekulare Chemie, 134, 299, (1970). 55 G.C. Berry, T.G. Fox Advances in Polymer Science, 5, 262, (1968). 56 P.G.J. De Gennes Chem. Phys., 55, 572, (1971). 57 J.D. Ferry Viscoelastic properties of polymers, 3rd Ed., John Wiley & Sons, (1980). 58 T.H. Mourey, S.R. Turner, M. Rubinstein, J.M.J. Fréchet, C.J. Hawker, K.L. Wooley Macromolecules, 25, 2401, (1992). 59 C.J. Hawker, P.J. Farrington, M.E. Mackay, K.L. Wooley, J.M.J. Fréchet Journal of the American Chemical Society, 117, 4409, (1995). 60 S. Uppuluri, S.E Keinath,D.A. Tomalia, A. Donald, P.R. Dvornic Macromolecules, 31, 4498, (1998). 61 G.S. Grest, L.J. Fetters, J.S. Huang, D. Richter Advances in Chemical Physics, 94, 67, (1996). 62 P.D. Olmsted, S.T. Milner Macromolecules, 27, 6648, (1994). 55 63 P.G.J. De Gennes Phys. (Paris) 36, (1975). M. Doi, N. Kuzuu Polymer Science, Polymer Letters Edition, 18, 775, (1980). 65 D.S. Pearson, E. Helfand Macromolecules, 20, 822, (1984). 66 R.C. Ball, T.C.B McLeish Macromolecules, 22, 1911, (1989). 67 G. Kraus, J.T. Gruver Journal of Polymer Science, A3, 105, (1965). 68 G. Quack, J.L. Fetters Polymer Preprints (Am. Chem. Soc., Div. Polym. Chem.), 18, 588, (1977). 69 J.E.L. Roovers, W.W. Graessley Macromolecules, 14, 766, (1981). 70 J. Pannell Polymer, 12, 558, (1971). 71 N. Hudson, W.A. MacDonald, A. Neilson, R.W. Richards, D.C Sherrington Macromolecules, 33, 9255, (2000). 72 Perstorp Polyols Inc. 73 H. Ihre, A. Hult, E. Söderlind Journal of the American Chemical Society, 118, 6388, (1996). 74 Malmstroem, Eva; Hult, Anders Book of Abstracts, 210th ACS National Meeting, Chicago, IL, August 20-24, (1995). 75 Viscotek World Headquarters, 15600 West Hardy Road Houston, TX 77060. 76 Gallot-Grubisic, Z.; Rempp, P.; Benoit, H. Journal of Polymer Science, Polymer Letters Edition, 5, 753, (1967). 77 M. Stogiou, C. Kapetanaki, H. Iatrou International Journal of Polymers, Analysis and Characterization,7, 273, (2002). 78 A.M. Striegel, R.D. Plattner, J. L. Willett Analytical Chemistry, 71, 978, (1999). 79 S. Penceck, A. Duda, Macromolecular Symposia, 107, 1, (1996). 80 L. Garamszegi, T.Q.Nguyen, C.J.G. Plummer, J-A.E. Manson Journal of Liquid Chromatography & Related Technologies, 26, 207, (2003). 81 B.H. Zimm, W.H Stockmayer Journal of Chemical Physics, 17, 1301, (1949). 82 S. Mori Size Exclusion Chromatography, 111, (1991). 83 P.A Small Advances in Polymer Science, 18, 1, (1975). 84 H. Keul, H. Hocker Macromolecular Rapid Communications, 21, 869, (2000). 85 H.R. Kricheldorf, A. Mahler Journal of Macromolecular Science, Pure and Applied Chemistry, A33, 821, (1996). 86 H.R. Kricheldorf, J. Jenssen Journal of Macromolecular Science, Chemistry, A26, 631, (1989). 87 Y. Shibasaki, F. Sanda, T. Endo Macromolecules, 33, 3630, (2000). 88 K.J. Zhu, R.W. Hendren, K. Jensen, C.G. Pitt Macromolecules, 24, 1736, (1991). 89 S.L. Bennett, K. Connolly, E. Gruskin, Y. Jiang Patent Appl. EP0837084, (1998). 90 S. Sarel, L.A. Pohoryles Journal of the American Chemical Society, 80, 4596, (1958). 91 W. Richter, P. Mues, H.J. Buysch Patent De3418092, (1985). 92 T. Tabuchi, T. Fujii Patent Jp081340660, (1996). 93 M. Moller, F. Nederberg, L. S. Lim, R. Kange, C. J. Hawker, J. L. Hedrick, Y. Gu, R. Shah, N.L. Abbott Journal of Polymer Science, Part A: Polymer Chemistry, 39, 3529, (2001). 94 H.R. Kricheldorf, B. Weegen-Schulz, J Jenssen Makromolekulare Chemie, Macromolecular Symposia, 60, 119, (1992). 95 H.R. Kricheldorf, R. Dunsing, A. Serra I Albet Makromolekulare Chemie, 188, 2453, (1987). 96 F. Sanda, H. Sanada, Y. Shibasaki, T. Endo Macromolecules, 35, 680, (2002). 64 56 97 C.A.P. Joziasse, H. Grablowitz, A.J. Pennings Macromolecular Chemistry and Physics, 201, 107, (2000). 98 W.W. Yau, D. Gillespie Polymer, 42, 8947, (2001). 99 J.K.F Tait, H.G.M Edwards, D.W. Farwell, J. Yarwood Spectrochimica Acta Part A, 51, 2101, (1995). 100 R.E. Lyon, K. E Chicke, S.M. Angel Journal of Applied Polymer Science, 53, 1805, (1994). 101 K. Sörensen, M. Johansson, E. Malmström, A. Hult Patent Swe9200564-4. 102 J. Roovers, J.E. Martin Journal of Polymer Science, Part B: Polymer Physics, 27, 2513, (1989). 103 J. Roovers, L.L. Zhou, P.M. Toporowski, M. van der Zwan, H. Iatrou, N. Hadjichristidis Macromolecules, 26, 4324, (1993). 104 I. Bodnar, A.S. Silva, R.W. Deitcher, N.E. Weisman, Y.H. Kim, N.J. Wagner Journal of Polymer Science, Part B: Polymer Physics, 38, 857, (2000). 105 R. Scherrenberg, B. Coussens, P. van Vliet, G. Edouard, J. Brackman, E. de Brabander, K. Mortensen Macromolecules, 31, 456, (1998). 106 B.M. Tande, N.J. Wagner, M.E. Mackay, C.J. Hawker, M. Jeong Macromolecules, 4, 8580, (2001). 107 T.G. Fox, P.J. Flory Journal of the American Chemical Society, 73, 1904, (1951). 108 O.B. Ptitsyn, Y.E. Eisner Sov. Phys. Tech. Phys., 4, 1020, (1960). 109 P.G. De Gennes, H. Hervet J de Physique, Lettres, 44, 351, (1983). 110 P. J. Flory Principles of polymerization, Cornell University press, Ithaca, (1953). 111 J. L. Fetters Polymer Preprints (ACS, Div Polym Chem), 18, 558, (1977). 112 C. Decker, K. Moussa Journal of Coatings Technology, 62, 55, (1990). 113 S. S. Lee, A. Luciani, J-A. E. Månson Progress in Organic Coatings, 38, 193, (2000). 114 H. H. Winter, F. Chambon Journal of Rheology, 30, 367, (1986). 115 F. Chambon, H.H. Winter Journal of Rheology, 31, 683, (1987). 116 S. S. Lee, A. Luciani, J-A E. Månson Progress in Organic Coatings, 38, 193, (2000). 117 S. B. Ross-Murphy Polymer 33, 2622, (1992). 118 C. Y. M. Tung, P. J. Dynes Journal of Applied Polymer Science, 27, 569, (1982). 119 H. H. Winter Polymer Enginering Sciience, 27, 1968, (1987). 120 B. Lebedev, A Yevstropov, Macromol. Chem., 185, 1235, (1984). 121 M. Johansson, E. Malmström, A. Jansson, A. Hult Journal of Coating Technology, 72, 49, (2000). 57 APPENDIX A H n H O O H n O H O O O O O H H O H H O O n O O O n n O O O n H n O O HO O O O O O O O O O O O O OH O O O O O O O O O O O O O O n O O O H H O O O O H O O n O H O O O n O n O O O O n O O O H O n O O H O O n n H Boltorn-PCL H n O O O n O O O O O O O n O H O O O O O O O O n O H O O O H n O O O O O n H O O O O n O O O O O H O O O O O O O O O O O O O O O O n O O n O O O O H O O n O H O O n O O O O O O O H O O O n n O O nO O H O H H H H n H O H O H n O H O O n O O H H O O O O n O O n O O H n O n O O O O O O n H O O O O n O n O O O O O O O O O H O O O n O H O O n O O O O O O O n O O O O O O O O O n H n H H Dendrimer-PCL n H H H n O n H n H O n O O O O H H O O O H O O O O n O O O O O O O O H O O O OO O n n O O O O O O O O O O O O O O O O n O O O O H O O O O O O O O H n O H n O O O O O O O O O O O O O O O O O O O O H H O n O O O O O O n O O n n H H Dendron-PCL H n O O O O O H n O O n O O O O H O O O O n O O n H Linear PCL H APPENDIX B Boltorn-PCL DP, DP, 1H- Mw, 1H-NMR -1 Mw, SEC Mw/Mn -1 aim NMR (g mol ) (g mol ) 5 7 10 12 15 20 25 30 35 40 45 50 50 55 55 70 5 8 10 13 16 22 22 32 36 40 46 51 54 55 56 79 21 900 32 800 40 100 49 300 62 000 84 000 84 000 120 500 135 100 149 700 171 600 189 900 200 800 204 500 208 100 292 100 29 500 43 100 50 800 66 700 72 200 99 400 107 100 126 800 144 200 168 000 199 800 193 900 187 700 220 500 216 100 279 900 Mw, SEC η0 Mz, -1 (g mol ) (Pa s) 2.99 3.38 3.36 3.16 3.32 3.11 3.68 6.39 5.25 6.92 7.58 8.45 9.88 7.62 8.35 7.68 54 400 82 200 90 300 118 000 124 700 189 200 199 100 237 000 271 000 328 900 420 600 380 600 365 900 410 400 419 300 545 900 1.18 1.32 2.48 4.24 4.69 10.3 13.8 21.0 45.0 79.8 100 135 129 235 137 460 Mw/Mn Mz, η0 Dendrimer-PCL DP, DP, 1H- Mw, 1H-NMR -1 -1 aim NMR (g mol ) (g mol ) 10 12 15 18 20 25 30 35 40 45 60 15 14 14 21 24 30 37 42 49 51 51 43 800 41 100 41 100 60 300 68 500 84 900 104 000 117 700 136 900 142 300 142 300 32 300 39 400 38 200 58 400 67 600 86 200 94 300 96 500 116 500 119 500 114 100 -1 1.35 1.43 1.43 1.50 1.18 1.31 1.33 1.50 1.60 1.56 2.00 (g mol ) (Pa s) 36 500 45 300 43 900 67 720 76 600 102 700 114 600 113 500 138 800 141 900 143 400 1.34 3.18 3.30 6.10 6.85 12.2 38.3 44.0 47.0 63.0 65.0 Dendron-PCL DP, DP, 1H- Mn, 1H-NMR -1 Mw, SEC Mw/Mn -1 aim NMR (g mol ) (g mol ) 10 13 18 15 17 20 20 20 25 35 37 40 80 11 14 15 16 19 20 21 22 23 35 39 41 81 11 000 13 700 14 600 15 500 18 300 19 200 20 100 21 000 21 900 32 900 36 500 38 400 74 900 11 900 14 600 15 300 16 400 18 300 20 400 22 000 22 700 22 200 32 600 36 000 38 700 65 400 Mw, 1H NMR Mw, SEC η0 Mz -1 (g mol ) (Pa s) 1.05 1.15 1.13 1.11 1.14 1.14 1.16 1.17 1.25 1.28 1.68 1.41 2.02 12 900 16 000 16 600 17 500 19 800 22 100 23 900 25 100 25 300 36 900 45 600 46 600 88 400 1.05 1.73 1.58 2.10 2.17 2.66 3.85 5.40 6.00 12.0 40.0 46.0 505 Mw/Mn Mz, η0 Linear-PCL DP, DP, 1H -1 -1 aim NMR (g mol ) (g mol ) 14 15 16 20 20 22 24 30 50 40 50 54 60 66 60 70 80 90 100 110 190 180 200 17 17 19 21 24 25 25 35 45 46 52 55 62 66 54 72 82 96 106 120 183 184 202 2 160 2 160 2 390 2 620 2 960 3 070 3 070 4 210 5 350 5 470 6 150 6 490 7 290 7 750 6 380 8 400 9 570 11 120 12 300 13 900 21 100 21 200 23 300 2 000 2 060 2 210 2 420 2 810 3 080 3 180 4 380 5 150 5 170 6 290 6 230 7 050 7 620 7 480 9 500 10 800 12 900 13 300 15 800 24 200 24 800 28 000 1.19 1.15 1.17 1.10 1.18 1.30 1.18 1.25 1.11 1.13 1.18 1.22 1.25 1.13 1.26 1.27 1.30 1.37 1.29 1.43 1.46 1.54 1.65 -1 (g mol ) (Pa s) 2 340 2 330 2 540 2 710 3 220 3 810 3 660 5 210 5 830 5 750 7 210 7 300 8 370 8 430 8 920 11 400 13 300 16 300 16 300 20 500 31 900 33 900 39 800 0.182 0.198 0.210 0.247 0.327 0.364 0.420 0.777 1.10 1.11 1.69 1.81 2.16 2.70 2.76 4.90 7.90 13.0 13.7 26.0 120 134 215 APPENDIX C OH HO O HO OH O O OH OH HO O O O O O O O O O O OH O O OH OH O OH OH O O O HO HO OH O O O O O O O O O O O O O O O O O O O OH O O O OH OH O O OH HO O O O HO OH O O HO OH O O O OH O O Hyperbranched polymer Boltorn H30 OH O O HO OH OH O O O NPC Catalyst OH O O OH n HO O O O O O O n n O O O O n O O O O O O O O n O O O n O O HO O n O O O O O O O O O O O O O O O O n O n OH O OH O O O O OH O O n O O O OH O O O O n OH O O n O O O O O O O n O O O OH O HO O O O O O O O O O O O O O O O O O O O O O n O O O O O O O O O O OH O O O O O O O OH n O O O O O O O O O O O O O OO O n HO O n O HO OH O O O O O O O O O OH O O O O O O O O O O O O O HO O O O OH O O O HO n O O O O O O O HO O OH O O OH OH Synthetic Scheme for Boltorn-PNPC OH
© Copyright 2026 Paperzz