Xiaolu Chena,
Hui Suna,
Jian Xub,
Xia Han*a,
Honglai Liua and
Ying Hua
aKey Laboratory for Advanced Materials and Department of Chemistry, East China University of Science and Technology, Shanghai 200237, China. E-mail: xhan@ecust.edu.cn; Fax: +86-216-425-2922; Tel: +86-216-425-2922
bShanghai Institute of Measurement and Testing Technology, Shanghai 201203, China
First published on 7th October 2015
Thermo-responsive hybrid nanoparticles composed of silica-core and poly(N,N-dimethylaminoethyl methacrylate-co-N-isopropylacrylamide) P(DMAEMA-co-NIPAM) copolymer-shell were prepared through a one-pot surface-initiated atom transfer radical polymerization (ATRP) technique. The well-defined core–shell hybrid nanoparticles with copolymer shell of uniform thickness were revealed by transmission electron microscopy (TEM). The thermo-responsive behavior of the hybrid nanoparticles in aqueous solutions was evaluated through combined techniques, including ultraviolet-visible spectrophotometer (UV-vis) and dynamic light scattering (DLS) analysis. Interestingly, pH-modulated LCST behavior with diverse aggregation processes can be observed. Specifically, the random copolymer grafted nanoparticles presented an LCST behavior with one-step transition process of shrink in acidic solution, a double LCST behavior with three-step transition process of shrink–shrink–aggregation in neutral solution, and a double LCST behavior with two-step transition process of assembly-shrink/aggregation in basic solution. The difference was attributed to the pH-modulated imbalances of electrostatic repulsion and hydrophobic interaction of the attached copolymer chains. Overall, these results disclose that pH and temperature can act as efficient modulators for the programmable control and fine-tuning of the morphology and aggregate size of the core–shell functionalized nanoparticles.
Incorporating different monomers which have thermo-responsive properties with LCST and/or UCST to be copolymers will give an opportunity to form new multi-responsive systems with largely extended diversity and flexibility of the thermo-responsive behavior. These multi-thermo-responsive systems usually contain polymers that exhibit different LCSTs,17–20 or both LCST and UCST21–23 in aqueous solutions. Usually, the phase transition behavior of thermo-responsive systems can be tuned by the chain length and the chemical composition of polymers, the ionic strength, the solvent polarity and the solution pH.24–29 If pH sensitive moieties contained, the system is expected to present pH-tunable phase transition behavior. Changing pH is a simple and effective way to tune the thermo-responsive behavior and it may have potential value in biological applications.30–32 Large reports have focused on the pH-tunable phase transition behavior of bulk polymers in solution. Change of phase transition temperature33,34 or phase transition type35 and multiple phase transitions36 by simply adjusting the solution pH have been achieved. Savoji et al.37 studied the thermo-responsive behavior of random copolymers poly(N,N-propylacrylamide-co-2-(diethylamino)ethyl methacrylate) and found that the cloud point in the range of 68–13 °C was strongly dependent on the solution pH. Jiang et al.38 demonstrated that a multiple and reversible phase transition of poly(ethylene oxide)-b-poly(methoxydi(ethylene glycol) methacrylate-co-methacrylic acid) block copolymers can be realized through adjustment of the solution pH. In our previous work35 the thermo-response of block copolymers, poly(ethylene glycol) methyl ether-b-poly(N,N-dimethylaminoethyl methacrylate) (mPEG-PDMAEMA), from no response in acidic media to an LCST transition in neutral media and an LCST and UCST transition in basic media was observed. While rare example about pH-modulated phase transition behavior of surface grafted polymers was reported, especially for the diverse aggregation behaviors derived from the synergistic effect of pH and temperature. Several groups39–41 reported the size of PDMAEMA-modified nanoparticles in aqueous solution was highly pH-dependent. PDMAEMA grafted hollow mesoporous silica nanoparticles was synthesized by Yu et al.42 and a good pH-controlled release behavior was observed with PDMAMEA chain as a gatekeeper. Yang et al.43 achieved the “on–off” switchable drug release system by utilizing the pH-responsive property of poly(2-(diethylamino)ethyl methacrylate)-b-poly(N-isopropylacrylamide) (PDEAEMA-b-PNIPAM) coated mesoporous silica nanoparticles. Matsumoto et al.44 reported a pH-tunable thermo-responsive aggregation behavior of a poly(N-isopropylacrylamide-co-acrylic acid) conjugated protein nanoparticle system, which may be useful in drug delivery. Zhang et al.45 synthesized asymmetric polymer grafted silica nanoparticles with one hemisphere coated with PNIPAM and the other coated with block copolymer PNIPAM-b-PDMAEMA. They claimed this polymer/inorganic nanocomposite presented UCST in pH 4 to LCST transition in pH 7 and pH 9. But the phase transitions were less obvious through UV-vis spectroscopy and there needs a detailed discussion about the reason. A pH-tunable thermo-responsive behavior of PDMAEMA grafted silica nanoparticles was reported by Dong et al.46 They found that the LCST of the system decreased with the increasing of the solution pH, which was explained by the electrostatic repulsion of protonated PDMAEMA in low pH.
In addition, a study of the detailed phase transition process was important to gain a better understanding of the thermo-responsive behavior. It was found that the thermo-responsive behavior of surface modified polymers was not so coincident with that of corresponding bulk polymers. That may be accounted for the confinement of the polymer chains on the surface and the steric hindrance among the crowded polymer chains.47,48 Chakraborty et al.49 reported that gold nanoparticles grafted PNIPAM presented slower aggregation kinetics compared with the bulk PNIPAM. The phase transition process of bulk polymers with pH-modulated thermo-responsive property was relatively simple. It was about the transition between unimers, micelles and aggregates through changes in the degree of ionization altered by pH. While the pH-modulated transition processes of polymers on surface with more flexibility and diversity need investigation.
In this paper, two thermo-responsive polymers, PDMAEMA and PNIPAM, were used to decorate the silica nanoparticles by one-pot surface-initiated atom transfer radical polymerization (ATRP) technique. As PDMAEMA is a pH-dependent thermo-responsive polymer and PNIPAM has an LCST around 32 °C, the hybrid nanoparticles are expected to present a pH-modulated thermo-responsive behavior. This study may help us gain a better understanding of the phase behavior of copolymer grafted silica nanoparticles and their tunable thermo-responsive behavior with pH.
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Scheme 1 Synthesis of SiO2-g-P(NIPAM-co-DMAEMA) silica nanoparticles by one-pot surface initiated ATRP. |
FTIR spectra and TGA were conducted to confirm the successful polymerization process. Amide moieties introduced by BIBB were verified by the absorption at 1536 cm−1 (Fig. 1b), as compared to that of bare silica nanoparticles (Fig. 1a). The characteristic absorptions at 1732 cm−1 (ester carbonyl group) (Fig. 1c–e) and 1665 (amide I band), 1536 cm−1 (amide II band) (Fig. 1d and e), suggested the presence of PDMAEMA and PNIPAM respectively. TGA results were shown in Fig. 2A. The difference in the weight retentions between SiO2, SiO2–NH2 and SiO2–Br indicates the successful functionalization of each step. A more direct comparison on the organic content of various samples is shown in Fig. 2B, which is obtained from the weight loss in the temperature range of 115–600 °C in Fig. 2A. After polymerization, an obvious increase in the organic content of 40.8%, 55.3%, and 64.8% for SiO2-D100, SiO2-N50D50 and SiO2-N83D17 systems, respectively, can be seen. It is suggested that NIPAM is prone to be initiated from the silica surface through ATRP as compared to DMAEMA.
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Fig. 2 (A) TGA curves for (a) SiO2, (b) SiO2–NH2 (c) SiO2–Br, (d) SiO2-D100, (e) SiO2-N50D50 and (f) SiO2-N83D17. (B) Organic content of the resultant silica nanoparticles. |
The morphology of the SiO2-g-P(NIPAM-co-DMAEMA) nanoparticles was investigated and observed using XPS and TEM. After polymerization, an obvious increase in N and C content, and a disappearance of Si peak were observed (Fig. 3a), indicated the coverage of polymers on the surface. For polymer functionalized silica nanoparticles, the C 1s spectra were fitted with the expected four contributions where four peaks at band energy of about 284.14 eV, 284.78 eV, 285.5 eV and 287.61 eV were assigned to –C,
–N,
–O and
O, respectively (Fig. 3b). The core–shell structure with a polymer shell thickness of approximately 10 nm of polymer grafted silica nanoparticles is clearly observed from the TEM images (Fig. 4b–d), in comparison with the TEM image of SiO2–Br (Fig. 4a).
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Fig. 3 (a) XPS spectra and (b) XPS high resolution C 1s spectra of SiO2-D100, SiO2-N50D50 and SiO2-N83D17. |
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Fig. 4 TEM images of (a) SiO2–Br, (b) SiO2-D100, (c) SiO2-N50D50 and (d) SiO2-N83D17. The scale bar in the inset is 50 nm. |
The transmittance of polymer grafted silica nanoparticles with changes in temperature in acidic solution is shown in Fig. 5A. As can be seen, all samples presented a small and smooth increase in transmittance upon heating, indicating the LCST behavior. In this condition, the PDMAEMA moieties were highly protonated due to its pKa of around 7.3.33 The grafted polymer chains were highly extended in the solution due to the strong inter/intra-chain electrostatic repulsion and the strong hydrogen bonding between polymer chains and water. With temperature rising, the extended chains started to shrink to be less stretched ones, ascribed to the intra- and interchain hydrophobic interactions. This can be proved by the DLS results as shown in Fig. 6A and B. Similar results about PDMAEMA grafted silica nanoparticles were reported elsewhere.46 Note that there was only a gentle increase in transmittance, which can be implied that the electrostatic repulsion limited the shrink, thus leading to a less obvious LCST transition. This transition cannot be identified solely from PNIPAM or PDMAEMA, but resulted from the thermo-response of both polymers. In addition, the sample with higher PDMAEMA content displayed a smaller change in transmittance, consistent with the stronger electrostatic repulsive interactions.
From Fig. 5C, SiO2-D100 in basic solution exhibited a typical LCST behavior with the LCST of about 64 °C, while the other two samples containing PNIPAM showed a broad and slight transition in a lower temperature range of 25–45 °C. Since the transmittance just reflects the collective behavior of all particles in macroscopic appearance, DLS measurement can sensitively monitor the statistical changes of the particles. Fig. 6E and F about the hydrodynamic diameters (Dh) and derived count rate as a function of temperature for SiO2-N50D50 and SiO2-N83D17 proved that there existed a two-stage transition in both systems ascribed to the collapse of PNIPAM at approximately 38 °C and that of PDMAEMA at approximately 58 °C, respectively. The significant increase in the derived count rate above 38 °C suggested the changes in interchain/interparticle association in this temperature range50 and a transition from multimodal to monomodal distributions in the Z-average size of the nanoparticles revealed a self-assembly process. Additionally, a sharp increase in the Dh and a slight decrease in the derived count rate were observed at temperature above 54 °C, indicating the collapse of PDMAEMA accompanied by immediate aggregation of nanoparticles. These results confirmed the double LCST behavior of PNIPAM and PDMAEMA grafted silica nanoparticles in basic solution with a two-step transition from assembly to shrink and aggregation.
A typical LCST behavior at about 75 °C in SiO2-D100 neutral solution was observed, which was similar to that in basic solution with the LCST of about 64 °C. However, P(NIPAM-co-DMAEMA) grafted silica nanoparticles showed very different behaviors in neutral solutions from those in basic solutions. Interestingly, a two-step drop in transmittance was clearly observed upon heating in SiO2-N83D17 solution (Fig. 5B). It indicated the double LCST thermo-responsive behaviors of polymer grafted silica nanoparticles resulted from the collapse of the PNIPAM and that of PDMAEMA. The first step in the temperature range of 35–46 °C was assigned to the collapse of PNIPAM while the second step in the temperature range of 65–71 °C corresponded to the collapse of PDMAEMA. Although it was not so evident in SiO2-N50D50 solution to give a narrow transition temperature range, there still existed a two-step drop in transmittance upon heating. The difference may be attributed to the random architecture and the mole ratio of the two components as reported in the block copolymer systems.51,52 Specifically, random copolymer with equivalent PNIPAM and PDMAEMA content resulted in more homogenous dispersion of both PNIPAM and PDMAEMA segments which led to the shortened segment length and the suppressed aggregation of each component. Thus, the broader and weaker phase transition of SiO2-N50D50 than that of SiO2-N83D17 was obtained. The DLS results give a detailed information about the transition process. Fig. 6C and D presented the three-step transition processes of SiO2-N50D50 and SiO2-N83D17 with two slight decreases and one evident increase in Dh. This transition can be identified to the collapse of PNIAPM, collapse of PDMAEMA and aggregation of the nanoparticles, respectively. Furthermore, a more obvious transition in Dh upon heating of SiO2-N83D17 was coincident with the results from turbidity measurement as shown in Fig. 5B.
The size of the polymer grafted silica nanoparticles in aqueous solution was not only temperature dependent but also pH dependent. In order to verify the effect of pH, sample SiO2-N33D67 with more PDMAEMA content was chosen to examine the pH dependent hydrodynamic diameters at 25 °C, as shown in Fig. 7. The Dh decreased from 800 nm to 180 nm with the increase of pH value from 3.0 to 9.0. Similar to the reasons discussed above, it was also attributed to the competition between the inter/intra-chain electrostatic repulsion of the highly protonated PDMAEMA moieties at low pH and the hydrophobic interaction of the gradually deprotonated PDMAEMA at higher pH. For the samples with less PDMAEMA component, similar trend can be observed with smaller decrement (see ESI, Fig. S1†). This was consistent with the PDEAEMA-coated mesoporous silica nanoparticles reported by Sun et al.39
A proposed model for the aggregation behavior of P(NIPAM-co-DMAEMA) random copolymer grafted silica nanoparticles is shown in Fig. 8. Different transition behaviors of SiO2-g-P(NIPAM-co-DMAEMA) can be observed in aqueous media with different pH values. The pH-modulated variation of electrostatic repulsive interactions resulted in the interchain/interparticle association and disassociation and the delicate balance between them. In acidic solution, copolymer chains with high charge densities resulted in the strong electrostatic interchain repulsions and interparticle repulsions which led to a LCST behavior with only one-step transition process of the shrink of copolymers. It should be noted that the LCST was indistinguishable from that of PNIPAM or PDMAEMA and it was ascribed to the compromise of the phase transition of both polymer segments. A competition of the reduced interchain and interparticle electrostatic repulsion and the stronger intrachain association in neutral solution allowed a stable intermediate state of the two component segments to be bead-necklace morphology53 which led to the two-step collapse individually and then a further increase in temperature caused aggregation. While in basic solution, there was no electrostatic repulsion to disperse and stabilize nanoparticles as both PNIPAM and PDMAEMA collapsed upon heating and the hydrophobic interactions between dehydrated copolymers resulted in an immediate aggregation as soon as the PDMAEMA collapsed. SiO2-g-P(NIPAM-co-DMAEMA) in neutral and basic solution presented double LCST behaviors but underwent different transition processes, corresponding to a three-step transition from shrink to shrink to aggregation and a two-step process of assembly to shrink/aggregation, respectively. The former is attributed to the electrostatic repulsion and hydrophilic–hydrophobic balance, while the latter is attributed to only the hydrophilic–hydrophobic competitions.
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Fig. 8 Schematic illustration of the proposed aggregation behavior of modified silica nanoparticles SiO2-g-P(NIPAM-co-DMAEMA) in (a) acidic, (b) neutral and (c) basic solutions. |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c5ra13557e |
This journal is © The Royal Society of Chemistry 2015 |