Macromolecular Chemistry and Physics Full Paper Well-defined N-Isopropylacrylamide DualSensitive Copolymers with LCST ≈38 °C in Different Architectures: Linear, Block and Star Polymers Lorenzo A. Picos-Corrales, Angel Licea-Claverie,* Jose M. Cornejo-Bravo, Simona Schwarz, Karl-Friedrich Arndt Reversible addition-fragmentation chain transfer (RAFT) polymerization is used to prepare temperature- and pH-sensitive statistical copolymers with lower critical solution temperature (LCST) close to 38 °C at pH 7.4 based on N-isopropylacrylamide and methacrylic acid derivative comonomers with a pKa close to 6. Statistical copolymers are re-activated to prepare amphiphilic block copolymers and star polymers with cross-linked core. The LCST is maintained by varying the architecture; however, the LCST originated behaviour changes due to self-aggregation. Statistical copolymers and short block copolymers show complex aggregation, whereas midsize block copolymers and star polymers show shrinkage of aggregate dimensions. The pH of the medium has a profound impact on the self-assembling behaviour of the different polymer architectures. 1. Introduction Responsive water-soluble polymers have been extensively investigated for the development of “smart” macromolecules that respond to external stimuli. Such stimuli-responsive L. A. Picos-Corrales, Prof. A. Licea-Claverie Instituto Tecnológico de Tijuana, Centro de Graduados e Investigación, A.P. 1166, 22000 Tijuana, B.C., Mexico E-mail: aliceac@tectijuana.mx Prof. J. M. Cornejo-Bravo Facultad de Ciencias Químicas e Ingeniería, Universidad Autónoma de Baja California, Calzada Universidad No. 14418, 22300 Tijuana, B.C., Mexico Dr. S. Schwarz Department of Polylelectrolytes and Dispersions, Leibniz Institute of Polymer Research Dresden, Hohe Strasse 6, 01069 Dresden, Germany Prof. K.-F. Arndt Physical Chemistry of Polymers, Dresden University of Technology, 01062 Dresden, Germany Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim polymers exhibit a transition in physical/chemical properties under a change in pH or temperature.[1–4] Therefore, they have been proposed and partially tested as drugdelivery carriers to improve the efficacy and reduce the toxicity of pharmacological therapies. Polymer-drug conjugates with prolonged circulation times target tumours by the “enhanced permeation retention” (EPR) effect. Once in the tumour interstitium, the polymer-drug can only enter cells by the endocytic route. After endocytosis, the drug could be released in early or secondary endosomes by pHcontrolled hydrolysis (pH drops from physiological 7.4 to 5 ≈ 6 in endosomes or to 4 ≈ 5 in lysosomes) or specifically by enzymolysis in lysosomes.[5,6] For drug delivery applications, the thermal responsiveness, for example, “lower critical solution temperature” (LCST) of the polymers, needs to be tuned to human body conditions.[7–9] Poly(N-isopropylacrylamide) (PNIPAAm) has been the most studied thermoresponsive (also called thermosensitive) polymer. In water, it undergoes a sharp coil to globule transition turning the chain insoluble, followed by hydrophobic aggregation and phase separation wileyonlinelibrary.com DOI: 10.1002/macp.201100468 301 Macromolecular Chemistry and Physics L. A. Picos-Corrales et al. www.mcp-journal.de above 32 °C.[10,11] Calorimetric studies have shown that the process of phase separation is preceded by disruption of hydrogen bonding to water molecules.[12] The temperature range of the whole process may be narrow (discontinuous) or broad (continuous) arising from experimental conditions (non-equilibrium) or by specific polymer chain interactions with water. Furthermore, the process is reversible, which means that precipitated polymer redissolves upon cooling. This is a distinctive aspect that makes PNIPAAm different to natural thermosensitive polymers such as proteins that usually do not “renaturate” by cooling. And, finally, the phase transition temperature may show a hysteresis in cyclic heating–cooling experiments.[13] If the PNIPAAm chains are chemically attached (cross-linked) forming a network structure, the coil to globule transition of the single chains leads to a cascadelike contraction of the macroscopic network. The LCST of PNIPAAm can be reversibly adjusted by a change in the conditions of the aqueous environment: presence of salts, surfactants and so on.[14–16] However, for drug delivery applications the main method used for LCST adjustment is the non-reversible change of LCST by chemical modification of the polymer chain. The number of chemically introduced units into the polymer chain can be one (end functionalization or initiator functionalization),[17,18] or more (copolymerization).[3,10,17,19−31] Aiming to increase the LCST of PNIPAAm from 32 °C to above body temperature, copolymerization with hydrophilic monomers, containing carboxylic acids, amines or hydroxyls as substituents, were abundantly studied.[3,10,17,19–31] Some of those reported acid monomers are good candidates for adjusting the LCST to above body temperature at pH 7.4.[21,22,24,26] In comparison, the use of tertiary amine containing comonomers to increase the LCST of NIPAAm has being less successful because at those pH values (7–8) amines are usually not ionized.[17,27,31] The effect of polymer architecture on LCST is a subject that has not been targeted in deep in the literature. In the case of PNIPAAm chains, there are reports that show that a star polymer changes its LCST with increasing number of arms compared to linear PNIPAAm.[32,33] This change in LCST can be ascribed to the hydrophobic effect of end groups in the star arms of relatively low molecular weight. In the case of grafted PNIPAAm chains onto a hydrophilic or pH-sensitive polymer backbone, some authors report a change of LCST with the number of grafts,[31,34] whereas others do not find any change.[35,36] There are also reports on grafting of polyoxazoline side chains into a PNIPAAm backbone.[37] In this case, the LCST increased with increasing content on polyoxazoline grafts, but only when carboxylic acid groups were introduced by hydrolysis of methyloxazoline units. The finding is confusing for block copolymers. From seven references in which one block is PNIPAAm and the block copolymer 302 do not self-assemble below its LCST,[38–44] three reported no change in LCST compared to pure PNIPAAm (31 or 32 °C),[38,39,44] two slight changes (33 or 34 °C)[40,41] and two changes up to 44 °C.[42,43] In the case of block copolymers that self-assemble below its LCST to micelles or vesicles, all this materials showed an effect of the second or even third block into their temperature sensitivity.[45–48] In the case of self-assembled nanostructures and also in the case of nano/microgels,[49–53] the LCST behaviour of PNIPAAm do not result necessarily in aggregation and precipitation, in most cases a shrinkage of the nanostructure or a change of a simple micelle into more complex aggregated structures were observed. Occurrence of precipitation depends on the properties of the other components of the nanostructure and additional conditions such as pH and the presence of salts. In the case of nano/microgels, they change its “LCST” behaviour as a function of comonomer, similarly to random linear copolymers.[49–53] Starting from these literature reports, we try to make some preliminary statements that would be the starting point of our own studies: 1 2 3 Random copolymers, terpolymers and nano/microgels show a change in LCST behaviour as a result of a hydrophilic (increase) or hydrophobic (decrease) comonomer. Usually, a low content on comonomer (up to 15 mol%) is enough to make the change. Graft copolymers, diblock and triblock copolymers (not assembling below LCST): some report a change, others report a minimal change and, finally, some report no change in LCST. The rationale that we find is that a change is observed only when the molar content of PNIPAAm is below 50%. Increasing the PNIPAAm content results in diminishing the effect until it disappear (between 50 and 65 mol% of PNIPAAm). Self-assembled block copolymers (below LCST), form nanostructures that change its size or type as a function of temperature. This temperature (we call it LCST for simplicity) is shifted as effect of the second (third) polymer chain. In case that the molar ratio of PNIPAAm is well above 50 mol%, still a change in LCST can be found. As for all block copolymers, the change in LCST diminishes with increasing PNIPAAm content. We must emphasize that, for these preliminary statements, different kind of chemistries in the copolymers are compared, which may be an oversimplification. In our investigation, the versatility of the RAFT polymerization technique[54,55] was exploited to prepare different topologies with the LCST close to the human body temperature: linear (statistical) copolymers, linear block copolymers and star-copolymers. Statistical copolymers of NIPAAm with hydrophobic weak-acid comonomers were prepared with the goal of effectively adjusting the Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim www.MaterialsViews.com Macromolecular Chemistry and Physics Well-defined N-Isopropylacrylamide . . . www.mcp-journal.de temperature of phase transition to 38 °C at pH 7.4. On the other hand, as the weak-acid groups contained in the comonomers ionize depending on pH, the resulting LCST of the copolymers may be influenced by the pH which opens the possibility of dual temperature and pHtriggered drug delivery. Our goal polymeric materials are soluble at physiological conditions and capable of responding by both a slight temperature increase or by a pH decrease at the physiologically relevant pHs of 7.4 and 5.0, respectively. Furthermore, the question of the effect of the copolymer architecture on LCST behaviour can be answered more easily in our model system since only one type of comonomer is used for all architectures. Finally, the reversibility of the LCST behaviour in the different architectures was also studied. 2. Experimental Section 2.1. Materials The monomers, 2-methacryloyloxybenzoic acid (2MBA), 4-methacryloyloxybenzoic acid (4MBA) and 5-methacryloyloxypentanoic acid (5MPA) (Figure 1A) were synthesized according to literature reports.[56,57] The RAFT agents, 4-cyanopentanoic acid dithiobenzoate (CPADB) and 2-hydroxyethyl 2-phenylacetate dithiobenzoate (HPDB) were synthesized following previously reported procedures.[58,59] 4,4′-Azobis(4-cyanopentanol) (ACP) was also prepared as described in literature.[60] All other chemicals were purchased. N-Isopropylacrylamide (NIPAAm, 97%, Aldrich) was purified by recrystallization from n-hexane. 4,4′-Azobis(4cyanopentanoic acid) (ACPA, 98%, Fluka) was recrystallized from methanol. Styrene (St, 99%, Spectrum), hexyl acrylate (HA, 98%, Aldrich) and divinylbenzene (DVB, 80%, Aldrich) were purified by passing through an inhibitor remover column (Aldrich). pDioxane (ACS grade, Fermont), diethyl ether (ACS grade, Fermont) and tetrahydrofuran (HPLC grade, Aldrich) were used as received. 2.2. Polymerizations 2.2.1. Preparation of PNIPAAm and Statistical Copolymers Macro-CTAs were synthesized with prescribed molecular weights via RAFT polymerization. PNIPAAm-S(C⫽S)Ph was prepared with molar ratios monomer/CTA/initiator 283:1.0:0.2 and 50:1.0:0.2. Random copolymers were synthesized with various molar per cents of comonomers in order to optimize the LCST to 38–40 °C. Poly(NIPAAm-co-4MBAX)-S(C⫽S)Ph (X = 2, 5%) was synthesized using molar ratios of 283:1.0:0.2 and 50:1.0:0.2. Poly(NIPAAm-co2MBAY)-S(C=S)Ph (Y=5%, 7%, 10%, 15%) was prepared with molar ratio 283:1.0:0.2. Poly(NIPAAm-co-5MPAZ)-S(C⫽S)Ph (Z = 5%, 7%) was synthesized with molar ratios 283:1.0:0.4 and 50:1.0:0.4. Monomer, CPADB and ACPA were dissolved in p-dioxane using monomer concentration of 1.412 mol L−1 to prepare macro-CTAs with Mn > 20 000 g mol−1. Monomer, HPDB and ACP were dissolved in p-dioxane using monomer concentration of 3.0 mol L−1 to prepare macro-CTAs with Mn < 20 000 g mol−1. The reagents were added to an ampoule, solutions were degassed by three freeze–evacuate–thaw cycles and, afterwards, the ampoules were sealed under vacuum. Reactions were carried out with stirring at 70 °C (CPADB) and 80 °C (HPDB) for prescribed polymerization times. The reactions were stopped by freezing, ampoules were then opened. The p-dioxane was removed by rotary evaporation and the residual polymer was re-dissolved in acetone. Polymer solutions were precipitated into excess of cold diethyl ether for removing monomers and non-polymeric residues. The residual polymer was dissolved in acetone and reprecipitated in excess of cold diethyl ether. This procedure was repeated three times. The polymer was finally dried under vacuum at room temperature overnight. 2.2.2. Preparation of Block Copolymers Figure 1. Chemical structures of (A) monomers and (B) synthetic strategy used. www.MaterialsViews.com Block copolymers were prepared using styrene and hexyl acrylate for the second block. Molar ratio monomer/macro-CTA/initiator 22:1.0:0.2 and macro-CTA concentration of 20.0 mmol L−1 were used to prepare block Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim 303 Macromolecular Chemistry and Physics L. A. Picos-Corrales et al. www.mcp-journal.de copolymers of Mn < 10 000 g mol−1. Molar ratio 50:1.0:0.2 (HA), 100:1.0:0.2 (St) and macro-CTA concentration of 7.0 mmol L−1 were used to prepare Block copolymers of Mn > 15 000 g mol−1. Macro-CTAs were dissolved in p-dioxane before adding monomer and initiator. Solutions were added to an ampoule, then degassed by three freeze–pump–thaw cycles, sealed under vacuum and placed in a thermostated oil bath (70 °C) for 24 h. Polymer solutions were precipitated into excess of cold diethyl ether without removing the p-dioxane. In this way, residual monomers and also homopolymers were removed. The residual block copolymer was re-dissolved in acetone and reprecipitated in excess of cold diethyl ether. This procedure was repeated three times. The block copolymer was finally dried under vacuum at room temperature overnight. 2.2.3. Preparation of Star Polymers Star polymers have been prepared by “arm-first” RAFT method with cross-linking adapting a procedure described previously.[61,62] Different molar ratios of DVB:macro-CTA were studied for determining optimum conditions for star preparation. For preparing star polymers with PNIPAAm arms, PNIPAAm-S(C ⫽S) Ph with Mn,GPC = 28 100 g mol−1 (molar ratios 10:1, 15:1, 20:1) and Mn,GPC = 25 900 g mol−1 (molar ratios 25:1, 30:1, 35:1) were tested. On the other hand, for preparing star polymers with copolymeric arms a molar ratio of DVB:macro-CTA = 35:1 was used with poly(NIPAAm-co-5MPA5%) ( Mn,GPC = 26 700 g mol−1) and with poly(NIPAAm-co-4MBA10%) ( Mn,GPC = 21 000 g mol−1). ACPA was used as initiator and a molar ratio of macro-CTA:initiator was 5:1 in all cases. The reagents were dissolved in p-dioxane using macro-CTA concentration of 4.8 mmol L−1. Solutions were added to an ampoule and degassed by three freeze-evacuate-thaw cycles. Ampoules were sealed under vacuum and immersed in an oil bath at 70 °C for prescribed polymerization times (24, 36 or 48 h). The reactions were stopped by freezing, ampoules were then opened. Polymer solutions were precipitated with diethyl ether for removing DVB; the precipitate was collected and dried under vacuum at room temperature overnight. HPLC grade) for NIPAAm polymers and THF/CH3COOH (50:1)v for random copolymers were used as eluent at a flow rate of 0.5 mL min−1 at room temperature. Monodisperse polystyrene was used as calibration standard. GPC was equipped with a refractive index detector (Varian RI-4) and a tri-angle light scattering detector (MINI-DAWN, Wyatt). Dynamic light scattering (DLS) was used to determine the hydrodynamic diameters (Dh). Measurements were carried out at room temperature (25 °C) using a Zeta-sizer “nano-ZS” from Malvern Instruments (ZEN3500) equipped with a green laser operating at λ = 532 nm. The angle of measurement is 173o (backscattering) and the size analysis was performed by CONTIN. The reported hydrodynamic diameters (Dh) were calculated using the Stokes–Einstein equation for spheres, as usual.[63] The scattering intensity as a function of temperature was also used for determining the LCST of the prepared polymeric materials. The hysteresis of the LCST behaviour at different pH values was also studied for selected polymers. For these studies a Zeta-sizer “Nano-S” from Malvern Instruments (ZEN1600) equipped with a red laser operating at λ = 632.8 nm and an angle of measurement 173o was used. The size analysis was performed at different temperatures using 3 min equilibrating time at each temperature in the heating cycle followed by 10 min equilibrating time at each temperature in the cooling cycle. The reported Dh values are the maxima in size distribution by intensity from CONTIN analysis and where calculated as described above. The shrinking temperature (Ttr) is reported as the temperature for the definitive size drop, which corresponds within experimental error with the LCST of the system. The polymer concentration was 1 mg mL−1 for determination of LCST and for hysteresis studies on statistical copolymers, whereas it was 0.4 mg mL−1 for hysteresis studies on block copolymers and star polymers. The solutions were prepared, shaken for 12 h and stored overnight in refrigerator. Before measurement, they were filtered off using a 0.45 micron syringe filter for eliminating dust. 1H NMR spectra were recorded on a Varian, Mercury-200 MHz nuclear magnetic resonance instrument with CDCl3 or CD3OD as solvents and tetramethylsilane (TMS) as internal reference. 2.2.4. Fractionation of Star Polymers and Free Arms Separation of star polymers from linear polymers not attached to the star polymer (free arms) was carried out by polymer fractionation. The used procedure was as following: into a beaker containing a magnetic stir bar, the precipitated star polymer product (1 g) was dissolved in acetone (15 mL). Star polymer fraction was precipitated by dropwise addition of cold diethyl ether (15 mL) into the solution. The precipitate was collected and dried under vacuum at room temperature overnight. 2.3. Characterization Polymer yields were determined gravimetrically. The molecular weights, polydispersity index (PDI = Mw/ Mn) and radius of gyration (Rg) were determined by gel permeation chromatography (GPC) using a Varian 9002 chromatograph with a Phenogel 10 guard column (50 mm × 7.8 mm), a Phenogel 5 linear mixed bead column (300 mm × 4.60 mm) and a Phenogel 10 linear (2) mixed bed column (300 mm × 7.80 mm) in series. Tetrahydrofuran (THF, 304 3. Results and Discussion 3.1. Statistical Copolymers with LCST ≈38 °C RAFT polymerization of NIPAAm is well documented.[54,55,61] The kinetics of NIPAAm polymerization using 4-cyanopentanoic acid dithiobenzoate (CPADB) as RAFT agent in p-dioxane as solvent was reported previously.[61] By the addition of an acid comonomer with less than 15 mol% in the monomer mixture, we do not expect a strong influence on the kinetics. CPADB is a type of RAFT agent that also works very well for methacrylate-type monomers.[55] Table 1 summarizes experiments at different polymerization times adding to NIPAAm each of the three acid comonomers used in this investigation. As expected, the molecular weight increases with polymerization time while low polydispersities (PDI = Mw/Mn, also simply Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim www.MaterialsViews.com Macromolecular Chemistry and Physics Well-defined N-Isopropylacrylamide . . . www.mcp-journal.de Table 1. Preparation of random copolymers by RAFT with different acid comonomers. Random copolymer Poly(NIPAAm-co-5MPA5%) Molar ratios M/CTA/Ia) Reaction time [h] Conv.b) [wt%] Mn(calc.)c) [g mol−1] Mn(GPC) [g mol−1] Mw/Mn (PDI) 283:1.0:0.2 14 32 10 857 12 000 1.027 16 40 13 502 16 000 1.042 283:1.0:0.4 Poly(NIPAAm-co-4MBA5%) Poly(NIPAAm-co-2MBA15%) 283:1.0:0.2 283:1.0:0.2 13 50 16 808 24 700 1.156 15 72 24 080 29 900 1.176 17 73 24 410 30 100 1.152 19 71 23 750 31 800 1.230 12 44 14 950 22 600 1.213 14 63 21 280 28 300 1.084 16 74 24 950 34 800 1.088 12 35 12 870 20 500 1.039 14 51 18 625 24 800 1.039 16 72 26 180 30 300 1.022 a)Polymerizations at 70 °C and using a monomer concentration of 1.412 mol L−1; b)Conversions determined gravimetrically; c)Calculated molecular weights based on Equation (1) called dispersity) are mantained. The measured molecular weights by GPC correspond well with the calculated ones using the ideal RAFT equation: [M]0 Mn(calc) = · MW,i · Rw + MW,CT A fi · (1) [CT A]0 where fi is mole fraction of monomer i, Mw is the molecular weight of monomer i and Rw is the fraction of conversion. The typical RAFT behaviour for copolymerization experiments with 4MBA and 2MBA was observed, showing a linear increase of molecular weight with time maintaining a low polydispersity (see Supporting Information). The composition of the statistical copolymers prepared was determined by 1H-NMR in deuterated methanol a good solvent for all type of monomers. In the spectra, the signals of the acid comonomer can be fairly good seen and the composition was calculated by integration of selected protons as described in the Supporting Information. Table 2 shows a series of synthesized copolymers produced with the aim to get different compositions and molecular weights. In some cases, the acid comonomer content was higher as expected from the comonomer Table 2. Characteristics of random copolymers with acid groups. Random copolymer Mn(GPC) Mw/Mn [g mol−1] (PDI) NIPAAm content [mol%]a) LCST by DLS [°C] pH = 7.8 7.4 Dhb) [nm] 6.0 5.0 4.4 pH = 7.8 7.4 6.0 4.4 Poly(NIPAAm-co-5MPA5%) 31 800 1.230 95.0 – 40 34 28 23 – 12.5 7.9 9.6 Poly(NIPAAm-co-5MPA5%) 6600 1.009 90.0 – 38 34 – – – 3.1 – – Poly(NIPAAm-co-5MPA7%) 30 700 1.249 93.3 40 – – – 28 17.6 – – 19.7 Poly(NIPAAm-co-4MBA2%) 26 800 1.214 – – 34 – – – – 8.7 – – Poly(NIPAAm-co-4MBA5%) 35 400 1.224 88.2 – 38 32 – – – 8.6 7.8 – – – Poly(NIPAAm-co-4MBA5%) c) 17 200 1.012 90.0 – 40 32 – c) – – 7.0 Poly(NIPAAm-co-4MBA5%) 5600 1.007 88.0 43 38 36 – – 3.5 2.8 – – Poly(NIPAAm-co-2MBA5%) 38 700 1.538 – – 32 – – – – – – – Poly(NIPAAm-co-2MBA7%) 35 300 1.655 – – 34 – – – – – – – Poly(NIPAAm-co-2MBA10%) 45 400 1.293 – – 36 – – – – 10.7 – – Poly(NIPAAm-co-2MBA15%) 38 900 1.038 84.0 – 40 – – – – 7.8 – – a)Content was determined by NMR; b)Dh data for copolymers as determined by DLS at 26 °C; c)Data was determined at pH 7.0. www.MaterialsViews.com Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim 305 Macromolecular Chemistry and Physics L. A. Picos-Corrales et al. www.mcp-journal.de Figure 2. LCST of random copolymers: (A) LCST of poly(NIPAAm95%-co-5MPA5%) Mn = 31 800 g mol−1 at different pH values; (B) LCST as a function of 2MBA content in poly(NIPAAm-co-2MBA) at pH 7.4. mixture. This is an indication that the incorporation of the acid comonomer do not follow the rules for ideal copolymerization; however, determination of copolymerization parameters was out of the scope of this investigation. The penultimate column in Table 2 summarizes also the LCST values measured at different pH for the statistical copolymers prepared. For each type of copolymer, an LCST close to 38 °C at pH 7.4 was obtained at certain acid comonomer content. This LCST value was reproduced also for short block copolymers ( Mnbelow 7000 g mol−1). Furthermore, the LCST value decreases with decreasing pH value. This trend is clearly seen in Figure 2A. This means that by adding an acid commoner to PNIPAAm the LCST is pH dependent. This statement is not always valid and deserves clarification. The selection of the acid comonomers for this purpose was very important. An acid comonomer with a pKa value higher than that of acrylic acid (AA) or methacrylic acid (MA) was needed given the fact that the LCST of copolymers of NIPAAm with AA or MA are to high at pH 7–8.[21] We have chosen three acid comonomers with pKa values between 5 and 6, namely, 5MPA with pKa = 6.14,[57] 4MBA with pKa = 5.3[56] and 2MBA with pKa = 5.8.[56] Furthermore, all three acid comonomers contain hydrophobic moieties as spacer groups (see Figure 1). This results in the fact that they are water insoluble at pH values lower than 5. These comonomers introduce into the PNIPAAm chain both, hydrophobic interacting units as well as ionizable acid units. At pH value of 7.4, more than 90% of acid units are expected to be ionized; however, at pH 6 the degree of ionization decreases differently for each acid comonomer. This can be calculated using the Henderson–Hasselbach equation[64] 306 1 −α (2) α where α is the degree of ionization of the acid units. Therefore, at pH 6, 42% of 5MPA units are ionized, while 83% of 4MBA units are ionized. The LCST change from 38 °C (pH 7.4) to 34 °C (pH 6) for the short block poly(NIPAAm-co5MPA), while it change from 38 °C (pH 7.4) to 36 °C (pH 6), for the similar in size and composition poly(NIPAAm-co4MBA). This change is remarkable in view of a possible biomedical application of these copolymers. It means that these copolymers are expected to change from expanded state to collapsed state in the endosome, if they go through endocytosis into a cell. The change in ionization degree is more dramatic at pH 5, only 6.8% of acid units in 5MPA are ionized and the LCST drops below that of PNIPAAm. The hydrophobic effect from the spacer chains is overwhelming at this pH. For the comonomer 2MBA, which has a pKa value in between the other ones discussed, we study the effect of comonomer content on the LCST. In other words, how much of this comonomer is needed to attain an LCST value ≈38 °C at a pH 7.4. Figure 2B shows the results in a graph. Between 10 and 15 mol% of 2MBA is needed to attain an LCST of ≈38 °C at pH 7.4. For comparison, only 5 mol% of the 5MPA acid monomer is needed to attain the desired LCST. It implicates that the acidity constant is the most important factor affecting the LCST at given pH value; however, other aspects such as hydrophobic interactions from other groups in the monomer are needed to be taken into account to have a real prediction. In any case, it has been shown that all three comonomers chosen can shift the LCST of PNIPAAm at pH 7.4 to values close to 38 °C at a certain concentration in the statistical copolymer pKa = pH + log Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim www.MaterialsViews.com Macromolecular Chemistry and Physics Well-defined N-Isopropylacrylamide . . . www.mcp-journal.de between 5 and 15 mol%. In addition, the LCST decreases to lower values when the pH decreases. This can be expected for acid comonomers, as their ionization degree falls and their hydrophobic interaction contributions overwhelm the hydrophilic ones. This implies that these copolymers are soluble at physiological conditions and show a coil to globule transition with precipitation either by increasing the temperature or by a change to lower pH values. These materials are therefore double-sensitive statistical copolymers. 3.2. Block Copolymers with LCST ≈38 °C Temperature-sensitive amphiphilic PNIPAAm copolymers were studied shortly after the LCST behaviour on PNIPAAm was discovered.[65] The main interest of introducing a second hydrophobic block into a PNIPAAm chain is to be able to attain nanosized aggregates in aqueous systems capable of transporting in their interior biologically active molecules.[66,67] In this investigation, we chose a frequently used hydrophobic block: polystyrene, which is a glassy polymer; and a non-reported one for this purposes: poly(nhexyl acrylate), which is rubbery. Both monomers have been proved to successfully grow in RAFT polymerization conditions to form block copolymers with PNIPAAm.[68,69] It was our goal to get block copolymers with micelle forming capacity in water at pH 7.4. By chain extending the statistical copolymers described in the previous section with 5 to maximal 15 mol% of hydrophobic units, we expect to get micelles as expected theoretically in the literature for amphiphilic block copolymers.[70] Table 3 shows the resulting block copolymers with very low polydispersity as expected for a controlled radical copolymerization method, and with hydrophobic comonomer Figure 3. LCST behaviour of “short” block copolymers at different pH values: poly(NIPAAm83%-co-5MPA7%)-b-PSt10%, Mn = 8800 g mol−1 (, pH 7.4; , pH 6.0) and poly(NIPAAm78%-co-5MPA10%)-b-PHA12%, Mn = 9100 g mol−1 (, pH 7.4; Δ, pH 6.0). content within the chosen range. Short blocks ( Mn < 10 000 g mol−1) and mid size blocks (up to 35 000 g mol−1) were prepared successfully. More important, LCST values close to 38 °C were still achieved. However, the influence of pH on LCST is different and need to be discussed more in detail. Figure 3 shows the LCST determination by turbidity for two (short) block copolymers differing only in the hydrophobic block. As can be seen, the LCST values for both block copolymers are the same, and this is also true at two pH values: 7.4 and 6.0. Nevertheless the difference in LCST at different pH values is, compared with the statistical copolymer used in its preparation, Table 3. Characteristics of block copolymers. Block copolymer Mn(macro-CTA)a) Mn(block)a) Mw/Mn [g mol−1] [g mol−1] [PDI] PNIPAAm-b-PSt Composition Dh [nm] 1st/2nd block pH = 7.4 7.0 6.0 [mol%]b) – 38.8c) LCST by DLS [°C] 4.4 pH = 7.4 7.0 6.0 4.4 – – – 30c) – – – – – 44 – 30 – 19.3 – – – 44 – 30 – (86-6.2)/7.8 119 – – 87 37 – – 24 1.044 (82-12)/6 – 94.0 27.6d) – – C.S.e) 36d) – 1.042 (81-9)/10 – 42.6 34.0d) – – C.S.e) 38d) – 18 000 22 100 1.024 84/16 poly(NIPAAm-co5MPA10%)-b-PSt 6500 8800 1.097 (83-7)/10 14.9 Poly(NIPAAm-co5MPA10%)-b-PHA 6500 9100 1.067 (78-10)/12 Poly(NIPAAm-co5MPA7%)-b-PHA 30 700 35 000 1.320 Poly(NIPAAm-co4MBA12%)-b-PSt 18 000 21 300 Poly(NIPAAm-co4MBA12%)-b-PHA 17 200 20 100 a) Molecular weights determined by GPC; b)Composition determined by NMR; c)Data were determined in pure water; d)Data were determined at pH 5.8; e)Continuous shrinkage. www.MaterialsViews.com Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim 307 Macromolecular Chemistry and Physics L. A. Picos-Corrales et al. www.mcp-journal.de bigger. Furthermore, the LCST for block copolymers at pH 7.4 is higher and at pH 6 lower, than for the statistical copolymers. The difference can be caused by a different aggregation behaviour. A statistical copolymer behaves similarly as a linear PNIPAAm chain does, it shows a coil to globule transition at LCST followed by self-aggregation and precipitation. Amphiphilic block copolymers already show aggregation below the LCST. This aggregation behaviour depends on block copolymer composition and on environmental parameters such as concentration, pH, presence of salts and also temperature. Table 4 shows the measured hydrodynamic radii in water together with estimates of contour lengths (Lc) of block copolymers and end to end distances of similarsize polymer coils in good solvent (h). On the one side, it can be considered that an spherical micelle would have a diameter around two times h (or Lc) of the block copolymer chains (radius would be therefore close to h or Lc of the block copolymer). On the other side, a vesicle (also named polymersome) would be constructed with two double layers including space in the core for water; resulting in more than five times h or Lc of the block copolymer (radius 2.5 times h or Lc). However, because the extended chains calculated from Lc are unrealistic for amphiphillic blockcopolymers in water, we took h as the best estimate. Therefore, we postulate the aggregates described in the last column of Table 4. Both short blocks studied form micelles below the LCST; when the temperature is increased above the LCST a coil to globule transition of the PNIPAAm copolymeric blocks would result in a change in the self-aggregation behaviour of the micelles. If the micelles are not very stable, they may disrupt to form bigger, more stable aggregates such as worms and vesicles; and they may finally precipitate; but if they are stable they can also shrink in its size without forming bigger structures. In the case of the short blocks, it is evident that their micelles are not very stable because the turbidity increases rapidly and they finally precipitate. However, the additional energy required to disrupt the micelles has the effect that the LCST is shifted to higher temperatures at pH value of 7.4 where the acid comonomer groups are almost completely ionized (≈95%). As less than half of the acid units are ionized (42%) at pH 6, the number of hydrophobic units from the non-ionized acid groups added to the hydrophobic block contribution leading to an LCST below that of the non-block copolymer. Figure 4 show the results of LCST for mid-size block copolymers. In this case, the size as Dh of block copolymers is plotted versus temperature to get a picture of the size of aggregates formed. Below the LCST, this block copolymers form micelles or slightly elongated micelles (see Table 4). A block copolymer PNIPAAm-b-PSt is used for comparison purposes. We can see that the size for the block copolymer with no acid comonomer doubles above the LCST. The block copolymers with acid 4MBA comonomer also increase it size above the LCST at pH 5.8, whereas at pH 7.4 and pH 7.0 they do not show a clear LCST up to 50 °C; however, its aggregates shrink continuously by heating (see Supporting Information). At pH 5.8, the LCST was measured to be between 36 and 37 °C. By comparison with statistical copolymers containing 4MBA units, we Table 4. Characteristics of aggregates formed by block copolymers in water Mn (block)a) [g mol−1] Contentb) [mol% 1°/2° block] Rhc) [nm] Lcd) [nm] he) [nm] Aggregate typef) 22 100 84/16 19.4g) 49.9 15.1 Micelleg) poly(NIPAAm-co5MPA10%)-b-PSt 8800 (83-7)/10 7.45h) 18.9 7.1 Micelleh) Poly(NIPAAm-co5MPA10%)-b-PHA 9100 (78-10)/12 9.65h) 17.4 7.1 Micelleh) Poly(NIPAAm-co5MPA7%)-b-PHA 35 000 (86-6.2)/7.8 59.5h) 43.5i) 72.0 15.4 Vesicleh) Vesiclei) Poly(NIPAAm-co4MBA12%)-b-PSt 21 300 (82-12)/6 47.0j) 13.8k) 43.8 15.1 Vesiclej) Micellek) Poly(NIPAAm-co4MBA12%)-b-PHA 20 100 (81-9)/10 21.3j) 17.0k) 39.8 13.2 Micellej) Micellek) Block copolymer PNIPAAm-b-PSt a) Molecular weights data were determined by GPC, THF was used as eluent; b)Content was determined from NMR; c)Rh data were determined by DLS at 25 °C; d)Lc (contour length), equal to the product of overall degree of polymerization times the contribution of one monomer repeat unit to the contour length, which is 0.254 nm[71]; e)h, the end to end distance of a coiled polymer chain in a good solvent.[63] Rg = 1.78 Rh was used.[72] Comparative molecular weights PNIPAAm ( Mn = 37 000 g mol−1, Dh(THF) = 6.5 nm[62]; Mn = 26 720 g mol−1, Dh(THF) = 6.4 nm[61]; Mn = 21 020 g mol−1, Dh(THF) = 5.6 nm[61]; Mn = 12 000 g mol−1, Dh(THF) = 3.0 nm)[62] was used; f) Micelle radius ≈ h, ellipsoidal micelle between 1.5 and 2 times h and vesicle ≥3 times h; g)Data were determined in water; h)Data were determined at pH 7.4; i) Data were determined at pH 4.4; j)Data were determined at pH 7.0; k)Data were determined at pH 5.8. 308 Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim www.MaterialsViews.com Macromolecular Chemistry and Physics Well-defined N-Isopropylacrylamide . . . www.mcp-journal.de In general terms, although the LCST value from the statistical copolymer is kept close to human body conditions by amphiphilic block formation, we find specific effects from the ionization degree of the acid comonomer (major) in addition to the hydrophobic block contribution (minor), resulting in slightly higher (high ionization) or lower (low ionization) LCST values. Furthermore, because amphiphilic block copolymers form aggregates in water, the LCST behaviour is not equal to that of linear chains. Aggregate type and its stability may shift the transition temperature value (Ttr better describes what is happening than LCST). 3.3. Star Polymers with LCST ≈38 °C Figure 4. LCST behaviour of mid-size block copolymers at different pH values: PNIPAAm84%-b-PSt16%, Mn = 25 000 g mol−1 in pure water (), poly(NIPAAm82%-co-4MBA12%)-b-PSt6%, Mn = 24 500 g mol−1 in buffer pH 5.8 () and poly(NIPAAm81%-co-4MBA9%)b-PHA10%, Mn = 19 200 g mol−1 in buffer pH 5.8 (). find here an increased LCST at pH 5.8. For this acid comonomer, the ionization degree is 76% at pH 5.8, whereas at pH 7.4 a 99% ionization is attained. At both pH values, we have an overall hydrophilic effect of the comonomer. The hydrophobic PSt block seems to favour aggregation at slightly lower temperatures than the PHA block. The midsize block in Table 4 containing 5MPA as acid comonomer shows at pH 7.4 LCST values below that expected from its acid comonomer content, 7% of 5MPA should result in an LCST higher than for 5% 5MPA (40 °C) but is not. This result suggests that the aggregates formed (vesicles, Table 4) are not stable at pH 7.4 and easily rearrange to other structures. The behaviour of this block copolymer is discussed in detail in the last section of this paper. The use of RAFT copolymerization for the preparation of branched polymer structures relies on the competition between chain growth by block copolymerization of a divinyl monomer into the re-activated macro-CTAs (copolymeric NIPAAm arms) and the coupling of growing chains containing a number of divinyl units into branched structures. If the amount of divinyl monomer related to that of the macro-CTA is high, then an undesired macroscopic polymer network would be obtained. On the other extreme, if the amount of divinyl monomer is too low, diblock copolymers with some branches of poly(NIPAAm-co-acid comonomer) are obtained. A star polymer with crosslinked core is only obtained at conditions where the divinyl monomer content is enough for branching but not enough for a wall to wall macroscopic cross-linking. In previous studies, we found that the concentration of macro-CTA and divinyl monomer in the recipe plays an important role in this reaction.[61,62] Therefore, we fixed a macro-CTA concentration and swapped a range of DVB cross-linker to macroCTA ratio to find conditions for star polymer synthesis. The synthetic scheme is described in Figure 1, whereas in Figure 5A we show preliminary experiments performed Figure 5. GPC traces of crude products for the synthesis of PNIPAAm-PDVB stars after 24 h polymerization time: (A) Molar ratio DVB:macroCTA for (a) 30:1; (b) 25:1 and (c) 20:1. (B) Molar ratio DVB:macro-CTA (30:1) and star product after fractionation. www.MaterialsViews.com Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim 309 Macromolecular Chemistry and Physics L. A. Picos-Corrales et al. www.mcp-journal.de using PNIPAAm macro-CTA as a model system to fix the cross-linker to macro-CTA ratio. As we can see from the GPC traces, with increasing ratio of cross-linker to macroCTA the content on star polymer increases. Nevertheless, a large amount of non-coupled macro-CTA (arms) are found in the crude product. Further increase of the ratio to 35:1 increased more the GPC peak for the star product, whereas a 40:1 ratio resulted in a macro gel formation. In Figure 5B, GPC traces of the star product (30:1) before and after fractionation are shown and compared to the macro-CTA used for its synthesis. The star product is enriched; however, a shoulder towards lower molecular weights is still observed, suggesting that the purification process was not complete. Further fractionation did not improved the GPC chromatogram; however, when we studied the product by DLS, we obtain a narrow distribution of sizes. We can see this pictured in Figure 6 for the star product (after fractionation) poly(NIPAAm-co-5MPA)arms-PDVBcore. This measurement was performed in THF, a good solvent for both arms and core of the star. The average size is 17 nm. Furthermore, we can see in Figure 6 that the size distribution in water at pH 7.4 is broad and much bigger, an indication of selfaggregation of the star polymer. The average size in water is 45 nm. Table 5 show the results of characterization experiments on star polymer products prepared with three different type of arms: PNIPAAm and two PNIPAAm copolymers with acid comonomers having an LCST close to 38 °C. As we can see, the polymer products are polydisperse (PDI = 1.6 to 2) and the molecular weight increases, as compared with that of the macro-CTA, from 4 to 8 times, suggesting that 4–8 arms are incorporated in the star products; in fact, the number of arms should be higher because the determination of molecular weight of star products by GPC is not very reliable. Hydrodynamic volume of star polymers is contracted compared to linear analogs of the Figure 6. Size distribution by volume for poly(NIPAAm-co5MPA5%)arms-PDVBcore star polymer (35:1) by DLS: (a) macro-CTA in THF; (b) star in THF; (c) star in water at pH 7.4. same molecular weight, so the value of molecular weight obtained by GPC may be underestimated. The composition of the star polymers as estimated by NMR (spectra in Supporting Information) shows that DVB is incorporated in 11 mol% or less in the star polymers. Apparently, the content on DVB is lower in the case of the star products with copolymeric arms; however, the NMR determination for these polymer products was performed in deuterated methanol, a non-solvent for DVB, whereas in the case of PNIPAAm arms deuterated chloroform was used, which is a good solvent for DVB. This procedure was necessary for a better solvatation of the polymeric arms to determine the acid comonomer content in the star polymers. In any case, we have star polymer products, which can be confirmed by further determination of architecture parameters. For Table 5. Characteristics of star polymers in THF. Mn,star/Mn,arm Dh,star/Dh,arm Composition arm/core [mol%]e) Star polymer [Cros.:macroCTA] Mn(GPC)d) [g mol−1] Mw/Mn [PDI] Rgd) [nm] Rhd) [nm] PNIPAAmarms-PDVBcorea) [30:1] 136 800 1.947 10.7 8.7 5.276 3.164 89/11 Poly(NIPAAm-co5MPA5%)arms-PDVBcoreb) [35:1] 108 100 2.005 8.6 8.3 4.046 2.594 (89-7)/4 Poly(NIPAAm-co4MBA10%)arms-PDVBcorec) [35:1] 167 900 1.613 9.6 6.5 7.988 2.321 (85-10)/5 Prepared using PNIPAAm with Mn = 25 930 g mol−1, PDI = 1.093 and Dh(THF) = 5.5 nm; b)Prepared using P(NIPAAm-co-5MPA5%) with Mn = 26 720 g mol−1, PDI = 1.125 and Dh(THF) = 6.4 nm; c)Prepared using P(NIPAAm-co-4MBA10%) with Mn = 21 020 g mol−1, PDI = 1.010 and Dh(THF) = 5.6 nm; d)Data were obtained in THF at 25 °C for star with PNIPAAm arms and in THF:CH3COOH (50:1)v for star with random copolymer arms; e)Determined by 1H-NMR. a) 310 Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim www.MaterialsViews.com Macromolecular Chemistry and Physics Well-defined N-Isopropylacrylamide . . . www.mcp-journal.de Table 6. Architecture parameters for star polymers and its aggregates. ga,b) ρc) No. of armsd) Dh,e,f) [nm] Dh,(pH 7.4)f) [nm] Xaggg) LCSTh) [°C] PNIPAAmarms-PDVBcore [30:1] 0.667 1.229 ≈4 17.4 91.9 5 32 Poly(NIPAAm-co-5MPA5%)arms-PDVBcore [35:1] 0.367 1.036 10–12 16.6 66.8 4 40 Poly(NIPAAm-co-4MBA10%)arms-PDVBcore [35:1] 0.457 Star polymer [Cros.:macroCTA] 38i) 1.477 6–8 13.0 59.0 4 >40 34j) factors calculated related to linear polymers of PNIPAAm; first entry a polymer with following characteristics: ( Mn(GPC) = 60 500 g mol − 1 and Rg = 13.1 nm), second and third entry, following characteristics ( Mn(GPC) = 52 300 g mol − 1, Rg = 14.2 nm); b)Contraction factor calculated by the equation g = Rg2,star/ Rg2,lin; c)Calculated by the ratio: ρ = Rg,star/Rh,star.d)According to W. Burchard;[72] e)Data were obtained in THF for star polymer with PNIPAAm arms and in THF:CH3COOH (50:1)v for star polymer with random copolymeric arms; f)Dh was determined at 25 °C.g)Number of aggregates calculated from the formula Xagg = Dh(pH 7.4)/Dh(THF); h)LCST was determined by turbidity at pH 7.4; i)By DLS; j)By DLS at pH 7.0. a)Contraction example, it is well known that branched macromolecules show a lower viscosity than linear polymers of the same molecular weight. Furthermore, the contraction factors g (based on R g) and g′ (based on viscosity) can be related to the number of arms of a star polymer.[72] Viscosity results show that the star polymers have a lower intrinsic viscosity than linear counterparts (see Supporting Information). In Table 6, a series of parameters for the star polymers are shown. Results can be related to the number of arms in the star polymer. Taking the g factor and the ρ parameter in THF as described for star polymers in a good solvent.[72] We postulate that the number of arms goes from 4 in the star with PNIPAAm arms to between 6 and 12 for the star products with copolymeric arms. As expected, the hydrodynamic diameter (Dh) in THF is lower for the star polymers with more arms (copolymeric arms). The measurements of Dh in water at pH 7.4 show that star to star aggregation is occurring because the diameter is several times that of the star polymer in THF. The number of stars per aggregate is calculated to be 4 to 5 (Table 6). The LCST studied by turbidity shows that, in general, the star polymers kept the LCST of the polymeric arms, although for the star polymer with poly(NIPAAm-co-4MBA) arms the turbidity decreases showing only a local maxima around 36 °C (Table 6, last row and Figure 7). We must take into consideration that the star polymers self-assemble in water below the LCST of their arms. This aggregation process results from the highly hydrophobic nature of DVB units in their cores. The aggregates formed are relatively stable and do not precipitate further by increasing the temperature; therefore, the turbidity is not very much affected by temperature rise. For a more detailed discussion on this behaviour, we made size investigations by DLS in heating and cooling cycles, as is going to be discussed below. Preliminary conclusions are that the LCST of the polymeric arms are kept when star polymers are formed, however, the typical LCST behaviour—coil to globule transition followed by self-aggregation and precipitation—is not occurring. The core of the stars plays a role in changing the LCST behaviour but not the LCST value. Figure 7. LCST by turbidity for star polymers: (A) PNIPAAmarms-PDVBcore star polymer; (B) poly(NIPAAm-co-5MPA5%)arms-PDVBcore star polymer and (C) poly(NIPAAm-co-4MBA10%)arms-PDVBcore star polymer. www.MaterialsViews.com Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim 311 Macromolecular Chemistry and Physics L. A. Picos-Corrales et al. www.mcp-journal.de Figure 8. Hysteresis of LCST for poly(NIPAAm90%-co-5MPA10%), Mn = 6600 g mol−1 (, heating; Δ, cooling) and for poly(NIPAAm88%-co -4MBA12%), Mn = 5600 g mol−1 (, heating; , cooling). 3.4. Effect of Polymer Architecture in Reversibility of LCST Behaviour The next question we wanted to answer was if the LCST behaviour is reversible for all type of structures we prepared with PNIPAAm and copolymeric PNIPAAm units. In the literature, it is reported that linear PNIPAAm shows a hysteresis in its LCST behaviour of less than 2 °C,[13] and the authors demonstrate that the LCST cannot be fully reversible because of other transition states involved and strong interactions with water molecules. We take this report as starting point to compare the LCST behaviour by heating and by cooling of the materials prepared. The purpose was to see if the behaviour is similar to that of pure PNIPAAm, to see how is the effect of comonomer and also to see the effect of architecture, if any. First of all, the LCST behaviour of PNIPAAm at a concentration of 0.4 mg mL−1 at pH 7.0 shows a higher hysteresis than the one reported in the literature. At this polymer concentration, aggregation and precipitation is observed, while in the literature report they prevent this by studying a very low concentration of a high-molecularweight PNIPAAm.[13] In our case, the cooling down cycle shows that the precipitate formed, re-dissolves only after long time and after solvating of the PNIPAAm chain is good enough for solution without stirring (see Supporting Information). In Figure 8, we can se the comparison of heating and cooling curves for random copolymers of PNIPAAm with short chains. As we can see, the behaviour is similar to that of pure PNIPAAm: large hysteresis with formation of big size aggregates at temperatures above the LCST value. A similar trend was observed for other statistical copolymers. In the case of block copolymers, the situation is very different. First of all, we find that 312 Figure 9. Hysteresis of LCST for poly(NIPAAm83%-co-5MPA7%)b-PSt10%, Mn = 8800 g mol−1 at pH 6.03 (, heating; Δ, cooling) and at pH 5.1 (, heating; , cooling). hysteresis is small to negligible (less than 2 °C). Furthermore, it depends strongly on the aggregation behaviour of the block copolymers and aggregate type below its LCST. For example, in Figure 9 we can see the behaviour of a short block copolymer at two different pH values. In both cases, we see that the polymeric micelles formed at temperatures below the LCST aggregate into more complex and big structures above the LCST, and that these structures returned to the micellar structure by cooling down with a small temperature hysteresis. However, in Figure 10 we can see that the vesicles formed by the mid-size block copolymer do not further aggregate above Figure 10. Hysteresis of LCST for poly(NIPAAm86%-co-5MPA6.2%)-bPHAt7.8%, Mn = 35 000 g mol−1 at pH 4.4 (, heating; Δ, cooling) and at pH 7.6 (, heating; , cooling). Macromol. Chem. Phys. 2012, 213, 301−314 © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim www.MaterialsViews.com Macromolecular Chemistry and Physics Well-defined N-Isopropylacrylamide . . . www.mcp-journal.de Figure 11. Hysteresis of LCST for star polymers. Poly(NIPAAmco-5MPA5%)arms-PDVBcore at pH 7.5 (, heating; , cooling) and poly(NIPAAm-co-4MBA10%)arms-PDVBcore at pH 7.0 (, heating; Δ, cooling). its LCST; they shrink in an almost continuously fashion at pH 7.6, while at pH 4.4 they shrink and most likely change structure from vesicle to a micelle. In both cases, the behaviour seems to be fully reversible with a negligible hysteresis. Also in the case of a block copolymer showing no clear LCST, poly(NIPAAm-co-4MBA12%)-b-PHA at pH 7.0, the shrinkage of the aggregate was followed up to 70 °C and by cooling the aggregate size was recovered with no hysteresis (see Supporting Information). In the case of star polymers, we also find a shrinkage of the aggregated star ensemble by going through the LCST value of the arms (Figure 11); however, in this case the reversibility is not granted because a hysteresis of up to 2 °C is observed together with a high scatter in size change. In fact, the aggregated star ensemble is not recovered totally, showing clearly non-reversibility. 4. Conclusion RAFT polymerization is a methodology that allows for the preparation of statistical, block and star polymers with LCST close to 38 °C at pH 7 to 7.4. This can be achieved with different comonomers and also in different molecular weights, in our case using acid comonomers. Once a statistical copolymer is prepared with the wanted LCST by RAFT, the fact that it is a “living” polymer chain, in this case called a macro-CTA; allows that this chain can be reactivated to be used for the preparation of more complex polymer structures such as block copolymers and star polymers. The so prepared complex polymer structures maintain in general terms the set LCST; however, the fact that the complex polymer structures may self-aggregate under www.MaterialsViews.com specific conditions of concentration, pH and temperature, provoke important behavioural differences for complex polymer systems containing the same copolymeric chains. For example, the same block copolymer may form at a specific pH value, micelles that further aggregate and finally precipitate by heating above the LCST of the copolymeric temperature sensitive block; however, at another pH value it may form vesicles that shrink by heating above the LCST value of the copolymeric block changing its structure to a more stable micelle. Even if the transition temperature (Ttr) is not very different to the LCST from the copolymeric blocks, it is very important to study the overall effect for the application of the complex polymer structures. Star polymers show that Ttr close to the LCST of their copolymeric arms, however if they aggregate and precipitate or only shrink by heating, depends strongly on the core forming polymer. In our case, a highly hydrophobic core resulted in star self-aggregation even below the LCST of the copolymeric arms. Reversibility of the temperaturesensitive effect cannot be truly achieved: the behaviour of statistical copolymers is similar to a pure PNIPAAm chain, while for block copolymers surprisingly we found several cases where, judging on overall size only, reversibility was better than for a PNIPAAm chain. Self-aggregating star polymers prepared showed non-reversibility of the temperature transition behaviour. The main advantage of using acid comonomers with pKa values close to 6 for tailoring the LCST of PNIPAAm is that a change in pH value of the environment from 7 to 6 already results in a clear change in LCST, making all the polymeric materials prepared good candidates for further investigations aiming biomedical application. Supporting Information Supporting Information is available from the Wiley Online Library or from the author. Acknowledgements: L.A.P.-C. thank DAAD for financing his PhD sandwich program. We thank J. Alvarez-Sanchez for the synthesis of one sample. Technical support by I.A. Rivero and A. Ochoa (IT-Tijuana) and M. Mende (IPF Dresden) is gratefully acknowledged. This investigation was supported by CONACYT (Mexico) SEP2006-60792. Received: August 8, 2011; Revised: October 18, 2011; Published online: January 3, 2012; DOI: 10.1002/macp.201100468 Keywords: block copolymers; LCST, PNIPAM; RAFT; star polymers [1] E. S. Gil, S. M. Hudson, Prog. Polym. Sci. 2004, 29, 1173. 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