Instantaneous Drug Delivery of Magnetic/Thermally Sensitive
Nanospheres by a High-Frequency Magnetic Field
Ting-Yu Liu, Shang-Hsiu Hu, Kun-Ho Liu, Ren-Shiuan Shaiu, Dean-Mo Liu,* and
San-Yuan Chen*
Department of Materials Sciences and Engineering, National Chiao Tung UniVersity, Hsinchu, Taiwan, 300, Republic of China
ReceiVed May 10, 2008. ReVised Manuscript ReceiVed July 2, 2008
Novel dual-functional nanospheres composed of magnetic iron oxide nanoparticles embedded in a thermo-sensitive Pluronic F127 (F127) matrix were successfully synthesized by an in situ coprecipitation process. The nanospheres were characterized by X-ray diffraction, transmission electron microscopy, X-ray photoelectron spectroscopy, and Raman spectroscopy. Experimental observations indicated that the F127 was subjected to a rapid structural change when the magnetic phase caused rapid heating after a short exposure to a high-frequency magnetic field. During the field duration, considerable volume shrinkage of the nanospheres (2.3-fold diameter reduction) was detected. This has been translated to an instantaneous release of a drug, Doxorubicin (DOX), when the DOX was encapsulated within the nanospheres. Such a rapidly responsive release of the DOX from the nanospheres was due to an intimate contact between the nanomagnet and F127, where an effective thermal and mechanical transfer between core and shell phases efficiently took place in the presence of the magnetic field.
1. Introduction
Drug carriers that are responsive to external stimuli, such as temperature, pH, light, mechanical signal, electric field, and magnetic fields, have received great attention in recent years.1-9 A wide variety of materials, such as carbon nanotubes, dendrimers, biodegradable nanoparticles (poly(lactide-co-glycolic acid) (PLGA) or poly(lactic acid) (PLA)), lipid vesicles (micelles), and gold or magnetic nanoparticles have been employed as matrix materials to deliver drugs. Among them, magnetic nanoparticles (MNPs) provide more interesting opportunities since they can be effectively activated in a controllable manner through a noncontact stimulus,10as compared with other materials. Although gold nanoparticles also displayed a similar inductive heating ability by infrared light stimulus, the manipulation and heating ability of MNPs were superior to those of the gold nanoparticles. The ability of magnets to convert magnetic energy into heat by the hysteresis effect has been known for a long period of time;11for instance, the ability has been used as antenna material for inductive heating in antitumor therapy, but the efficiency has not been as
good as desired without combining inductive heating with drug delivery. In order to enhance the tumor-inhibition ability, the combination of the heat transfer and drug release in nanoparticles will be more interesting. In our previous work, we developed magnetic hydrogels (ferrogels)12-14and magnetically sensitive nanospheres for controlled drug release by a high-frequency magnetic field (HFMF).15,16However, the silica seems to be a thermally insensitive material, and it was believed that the nanostructure did not change with temperature increases. In order to accelerate the rate of drug release, a thermosensitive polymer was used in this system because it exhibited a huge volume change when the temperature was increased.17
A number of polymeric materials are known to exhibit a discontinuous change of properties when subjected to a tem-perature change.17-23 Some of these systems, e.g., thermor-eversible gels, have been based on the existence of a lower critical solution temperature (LCST), or critical micellization temperature (CMT), and have usually been applied as intelligent drug carriers.17-23Poly(N-isopropylacrylamide) (PNIPAAm), poly-(ethylene glycol)-poly(lactic acid)-polypoly-(ethylene glycol) tri-blocks (PEG-PLA-PEG), and poly(ethylene oxide)-poly-(propylene oxide)-poly(ethylene oxide) (PEO-PPO-PEO) * Corresponding author. Address: Department of Materials Sciences and
Engineering, National Chiao Tung University 1001 Ta Hsueh Road, Hsinchu, Taiwan 300, ROC. Telephone: 5712121ext. 31818. Fax: +886-3-5725490. E-mail:[email protected] (S.-Y.C.); deanmo_liu@ yahoo.ca (D.-M.L.).
(1) Kim, M. R.; Park, T. G. J. Controlled Release 2002, 104, 69–77. (2) Zhang, X. Z.; Wu, D. Q.; Chu, C. C. Biomaterials 2004, 25, 3793–3805. (3) Chiu, G. N. C.; Abraham, S. A.; Ickenstein, L. M.; Ng, R.; Karlsson, G.; Edwards, K.; Wasan, E. K.; Bally, M. B. J. Controlled Release 2005, 104, 271– 288.
(4) Lu, Z.; Prouty, M. D.; Guo, Z.; Golub, V. O.; Kumar, C. S. S. R.; Lvov, Y. M. Langmuir 2005, 21, 2042–2050.
(5) Qiu, Y.; Park, K. AdV. Drug DeliVery ReV. 2001, 53, 321–339. (6) Etrych, T.; Jelı´nkova´, M.; Øı´hova´, B.; Ulbrich, K. J. Controlled Release
2001, 73, 89–102.
(7) Chen, S. C.; Wu, Y. C.; Mi, F. L.; Lin, Y. H.; Yu, L. C.; Sung, H. W. J.
Controlled Release 2004, 96, 285–300.
(8) Murdan, S. J. Controlled Release 2003, 92, 1–17.
(9) Mamada, A.; Tanaka, T.; Kungwatchakun, D.; Irie, M. Macromolecules
1990, 23, 1517–1519.
(10) Kohler, N.; Sun, C.; Fichtenholtz, A.; Gunn, J.; Fang, C.; Zhang, M.
Small 2006, 2, 785–792.
(11) Kim, D. H.; Lee, S. H.; Kim, K. N.; Kim, K. M.; Shim, I. B.; Lee, Y. K.
J. Magn. Magn. Mater. 2005, 293, 320–327.
(12) Liu, T. Y.; Hu, S. H.; Liu, T. Y.; Liu, D. M.; Chen, S. Y. Langmuir 2006,
22, 5974–5978.
(13) Hu, S. H.; Liu, T. Y.; Liu, D. M.; Chen, S. Y. J. Controlled Release 2007,
121, 181–189.
(14) Liu, T. Y.; Hu, S. H.; Liu, K. H.; Liu, D. M.; Chen, S. Y. J. Controlled
Release 2008, 126, 228–236.
(15) Hu, S. H.; Liu, T. Y.; Liu, D. M.; Chen, S. Y. Macromolecules 2007, 40, 6786–6788.
(16) Hu, S. H.; Liu, T. Y.; Huang, H. Y.; Liu, D. M.; Chen, S. Y. Langmuir
2008, 24, 239–244.
(17) Choi, S. H.; Lee, J. H.; Choi, S. M.; Park, T. G. Langmuir 2006, 22, 1758–1762.
(18) Schmidt, A. M. Colloid Polym. Sci. 2007, 285, 953–966.
(19) Coughlan, D. C.; Quilty, F. P.; Corrigan, O. I. J. Controlled Release 2004,
98, 97–114.
(20) Bhattacharya, S.; Eckert, F.; Boyko, V.; Pich, A. Small 2007, 3, 650–657. (21) Li, Y. Y.; Zhang, X. Z.; Kim, G. C.; Cheng, H.; Cheng, S. X.; Zhuo, R. X.
Small 2006, 2, 917–923.
(22) Bae, K. H.; Lee, Y.; Park, T. G. Biomacromolecules 2007, 8, 650–656. (23) Desai, P. R.; Jain, N. J.; Sharma, R. K.; Bahadur, P. Colloid Surf., A 2001,
178, 57–69.
10.1021/la801451v CCC: $40.75 2008 American Chemical Society Published on Web 10/28/2008
In the present work, a dual-functional nanoparticle was developed by integrating a nanomagnetic core with a shell layer of thermosensitive hydrogel to encapsulate an anticancer agent. Inductive heat was generated in the presence of HFMF. When heated, the thermosensitive polymer collapsed around the iron oxide nanoparticles, inducing an accelerative drug release. In recent years, some researchers24-27 have reported that dual-functional drug carriers included magnetic/thermal sensitivity, but few reports emphasized controlled drug release using HFMF. In addition, raising the temperature of the drug carriers from the surrounding heat source has been insufficient; a better alternative would be to supply the heat source by the drug carrier, e.g., the inductive heating effect induced by HFMF to a magnet core. This type of drug carrier can have great potential for disease treatment.
Moreover, the use of a high-frequency magnetic stimulus can also achieve an “instantaneous” burst release of drug by rapid heating to induce an instant shrinkage of the F127 hydrogel. Choi et al.17reported that Pluronic/Heparin nanocapsules exhibit a 1000-fold thermally reversible volume transition when the temperature changes from 25 to 37 °C. The violent volume-shrinkage would induce rapid drug release. Therefore, the combination of magnetic and thermal properties would be a very interesting alternative for tumor therapy. Here, we developed a novel Pluronic/iron oxide MNP formulated by an in situ coprecipitation process and evaluated it as a drug carrier. The proposed synthesis process of F127-MNPs is depicted in Figure 1a and is characterized by transmission electron microscopy (TEM), X-ray diffraction (XRD), Raman spectroscopy, X-ray photoelectron spectroscopy (XPS), spectrofluorophotometry (PL), and dynamic light scattering (DLS). Thereby, we demonstrated an approach to form water-dispersible and magnetic/thermore-sponsive nanoparticles formulated with F127 and iron oxide nanoparticles, which can be applied to biomedical devices such as drug carriers.
2. Experiment
2.1. Procedures. Nanospheres of Pluronic F127 (F127) and MNPs (F127-MNPs) were synthesized using an in situ coprecipitation of Fe(II) and Fe(III) salts in the presence of Pluronic F127 (F127, Sigma). In this process, the optimum ratio of iron oxide precursor and F127 hydrogel was described: 0.05 g of F127, 5 mmol of FeCl3· 6H2O (Riedel-deHae¨n), and 2.5 mmole of FeCl2· 4H2O (Fluka) were dissolved in 50 mL of water while being vigorously stirred at 60°C. The dissolved solution was sonicated by a horn-type ultrasonic homogenizer (VC-500 W, Cole-Parmer Instruments, USA) operating at a constant frequency of 20 kHz for 10 min. Then, Pluronic F127/ iron oxide salt nanospheres were prepared, as shown in Figure 1-(a1) (where pure F127 nanospheres (appropriate size: 10-30 nm) were
made in a similar process with sonication). Later, the pH was adjusted to 10 by adding ammonia solution (33%) to the reactor while stirring. This was followed by heating to 60°C, where it remained for 30 min. After washing five times with phosphate-buffered saline (PBS, pH 7.4), subsequent filtering by Acrodisc syringe filters (Aldrich, diameter 25 mm, pore size 0.2µm), and vacuum-drying,
F127-MNPs were then successfully prepared, as shown in Figure 1a2. Doxorubicin (DOX, MW: 580, Sigma, USA), a well-known anticancer drug, was used as a model molecule. DOX was employed because of its amphoteric characteristics; it can dissolve in an aqueous environment (ca. 10 mg/mL) or in an organic solvent (high solubility in methanol and chloroform). For incorporation in the F127-MNPs, 2 mL of an aqueous solution of DOX (2 mg/ml) was added drop by drop to 3 mL of an aqueous dispersion of F127-MNPs (100 mg of particles in the 3 mL PBS solution) while stirring. Stirring was continued overnight at 4°C to allow the drug to disperse into the F127-MNPs (see Figure 1b1). Because the F127-MNPs exhibit swelling at lower temperatures (4°C), DOX easily diffused into the ferrospheres. Then, DOX was well encapsulated under 15°C (the collapsing state was at a higher temperature, which formed the protecting-like layer (skin layer) and prevented drug escape), as shown in Figure 1b2. Then, drug-loaded ferrospheres were separated from the unentrapped drug using a magnet. F127-MNPs were washed three times by being resuspended in distilled water and separated, as described above, using the magnetic field. The resultant samples were dialyzed by a dialysis membrane with an MW cutoff at 14 000 and stored at 4°C before the nanospheres were used.
2.2. Fluorescence and Brunauer-Emmett-Teller (BET) Measurement. Pyrene loading was studied in order to assess the temperature-dependent aggregation within the microgels. A stock solution of 1 mM pyrene in absolute methanol was prepared, from which 2µL was added to 3.0 mL of a 100 mg F127-shell MNPs
aqueous sample. The sample was then allowed to equilibrate for 24 h at 25°C. The excitation and emission spectra were recorded (24) Zhang, J. L.; Srivastava, R. S.; Misra, R. D. K. Langmuir 2007, 23,
6342–6351.
(25) Chen, S.; Li, Y.; Guo, C.; Wang, J.; Ma, J.; Liang, X.; Yang, L. R.; Liu, H. Z. Langmuir 2007, 23, 12669–12676.
(26) Deng, Y.; Wang, C.; Shen, X.; Yang, W.; Jin, L.; Gao, H.; Fu, S.
Chem.;Eur. J. 2005, 11, 6006–6013.
(27) Detlef, M. S.; Thomas, S. R. J. Magn. Magn. Mater. 2006, 302, 267–271.
(28) Bromberg, L.; Temchenko, M.; Hatton, T. A. Langmuir 2003, 19, 8675– 8684.
(29) Bromberg, L.; Barr, D. P. Macromolecules 1999, 32, 3649–3657.
Figure 1.Diagram showing the proposed synthesis process of F127-MNPs: (a1) F127/iron salts nanosphere formation by sonication; (a2) F127-MNPs formation after adding ammonia solution to pH ) 10. Proposed mechanism for drug encapsulation and delivery process of F127-MNPs by HFMF: (b1) drug diffuses into the nanospheres at lower temperature (4°C, swelling state); (b2) slight volume shrinkage and drug encapsulated in the nanospheres after slight heating to 15°C; (b3) sharp volume shrinkage with accelerative drug release under HFMF treatment.
using a spectrofluorophotometer (PL) [Kimmon, IK5552R-F, Japan]. A He-Cd laser (25 mW) was the excitation source. There were five vibrational peaks in the pyrene emission spectra. The ratio of the intensities of the first (372 nm) to the third (385 nm) vibrational peak (I372/I385) in the emission spectra of the monomer pyrene was used to estimate the polarity of the pyrene microenvironment.28,29
BET analysis (Quantachrome, NOVA 2000, USA) was conducted using N2gas absorption isotherms at 77 K, and the pore sizes were calculated following the Barrett-Joyner-Halenda (BJH) method.30 The nanospheres (0.5 g) were dried in vacuum conditions for 1 day before BET analysis. The sample was degassed for 2 h with a residual vacuum of 0.532 Pa following BET analysis.13,16
2.3. Drug Delivery Test. Drug release behavior of the F127-shell MNPs was investigated by applying an HFMF of 50-100 kHz and 15 kW externally. A cooling water system, copper coil, and HFMF generator were included. The hollow structure of the copper coil was made in order to facilitate cooling water to pass through for temperature control. The copper coil of HFMF was 8 loops, and the strength of the magnetic field was 2.5 k A/m.15,16 Similar equipment has been reported in the literature.31Because the HFMF generates heat around the copper coil during operation, it was kept at 25°C through a cooling water bath to prevent thermally induced interference from the environment. To measure the concentration of drug release, 10 mL of PBS containing 0.2 g of F127-MNPs was kept at 15°C in the water bath. The absorbance at 482 nm26was measured by a UV-visible spectrophotometer (8453, Agilent, USA) to determine the concentration of DOX released into the PBS.
3. Results and Discussion
3.1. Morphology and Characterization of F127-Shell MNPs. Morphology of F127-shell MNPs was examined by TEM (JEM-2010, JEOL, Japan). Figure 2a shows the TEM images of pure F127 nanospheres, displaying a ring-like structure, which was a phenomenon due to the block-copolymer (Pluronic F127)
self-assembly. After the precursors of Fe(II) and Fe(III) salts and the ammonia solution were added, iron oxide nanoparticles started to form by coprecipitation. Figure 2b shows that well-distributed F127-MNPs have a spherical geometry of 10-20 nm diameter. Moreover, under high-resolution TEM [Figure 2b1], the iron oxide nanoparticles were encapsulated in the interior region of F127 nanospheres, and it was a crystalline structure (inset, Figure 2b2). In addition, the selected area diffraction pattern of the F127-shell MNPs showed five planes, namely, [220], [311], [400], [511], and [440], indicating the presence of iron oxide nano-particles, as well as an amorphous phase, e.g., cloudy ring (see Figure 2b3). This again suggests that the iron oxide nanoparticles were encapsulated by F127 hydrogel.
Figure 3 shows the results of the XRD (M18XHF, Mac Science, Japan) of the F127 nanospheres and F127-MNPs. In Figure 3a, six diffraction peaks at 2θ ) 30.1°, 35.6°, 43.3°, 53.5°, 57.2°, and 62.9°were the characteristic peaks of the crystal plane, which (30) Rouquerol, F.; Rouquerol, J.; Sing, K. Adsorption by Powders and Porous
Solids; Academic Press: London, 1999.
(31) Derfus, A. M.; von Maltzahn, G.; Harris, T. J.; Duza, T.; Vecchio, K. S.; Ruoslahti, E.; Bhatia, S. N. AdV. Mater. 2007, 19, 3932–3936.
Figure 2.TEM image of the morphology of (a) pure F127 nanospheres and (b) distribution of F127-MNPs. (b1) TEM image of F127-MNPs nanospheres (iron oxide nanoparticles were encapsulated in the F127 nanospheres). (b2) High-resolution TEM image showing the crystalline condition of iron oxide in the F127 nanosphere. (c) Diffraction pattern of F127-MNPs.
Figure 3.Characterization analysis of F127 and F127-MNP nanospheres: (a) XRD; (b) Raman spectra.
These results were similar to those of the diffraction pattern of the TEM (cloudy ring), indicating that both phases were intimately contacted.
Raman spectra are potentially more useful than diffraction techniques to track subtle structural differences between the vibration frequencies of F127 and Fe3O4MNPs. Figure 3b shows that, although F127 hydrogels were surrounded with iron oxide nanoparticles, a significant difference between these phases can be recognized from the Raman spectra. Both 665 and 704 cm-1 bands, assigned to the characteristic band of Fe3O4,32 were attributed to the vibrational modes. These consisted of the stretching mode of oxygen atoms along Fe-O bonds (metal oxide bond), and four characteristic peaks at 492, 537, 603, and 709 cm-1were assigned to F127 nanospheres.33,34Furthermore, from the sample of F127-MNPs, six peaks, including the peaks from both F127 and Fe3O4MNPs, were observed where the two peaks of 492 and 537 cm-1 were almost combined to form a broad peak. This suggests that there was some interaction between metal oxide and the -OH group in the F127 when the iron oxide nanoparticles were formed inside the F127 hydrogel.
In addition, the change in chemical-binding energy in F127-MNPs was investigated via XPS (ESCALAB 250, Thermo VG Scientific, West Sussex, U.K.), equipped with Mg KR at 1253.6 eV at the anode. As illustrated in Figure 3c, the binding energy of O1swas detected from 526.0 to 538.0 eV, and the peak of iron oxide was at 530.0 eV.35This peak represented the metal oxide, which was reasonably consistent with peak reported in the literature, i.e., 528-531 eV. Also, the -OH group peak of pure F127 nanospheres was found in the 532.8 eV, which was similar to the report of Anderson et al.,36showing a highly ordered arrangement of ring-like crystallization of the F127 nanospheres. However, after incorporation into the iron oxide nanoparticles (F127-MNPs), the peak at 532.8 eV shifted to a lower energy, 532.4 eV, indicating that the ring-like crystallization of the F127 nanospheres had been deteriorated to an amorphous-like structure as a result of the presence of iron oxide nanoparticles. In the meantime, the peak of the metal oxide in the F127-MNPs shifted to a higher energy, i.e., from 530.0 to 530.3 eV, suggesting that some interactions occurred between the metal oxide and the -OH group in the F127 hydrogel when the iron oxide was formed inside the F127 hydrogel. Although the actual mechanism for the shift of the binding energy of metal oxide is unclear at present, it is believed that iron ions can be encapsulated by the F127 hydrogel. This hydrogel promoted a self-assembly of the iron oxide salt to form crystal structure while increasing solution pH
upon synthesis, and it thus accompanies some ion-ion interaction to change the binding energy of metal oxide.15
3.2. Hydrophilic/Hydrophobic Properties. Pyrene is poorly soluble in a polar environment, but it strongly emits radiation when it is self-aggregated or forms microdomains (i.e., micro-aggregates) in an aqueous solution.28,29,37The intensity ratio (I372/I385) of the first peak (372 nm) and the third peak (385 nm) of the fluorescence emission spectrum for pyrene has been shown to be sensitive to the polarity of the microenvironment.28,29The reason was that increasing the polarity of the medium induces an increase in the intensity of the first peak, I372, corresponding to the forbidden transition, while the intensity of the third peak, I385, corresponding to the allowed transition, remains unchanged.38 The ratio was higher in a polar medium; for example, in water, I372/I385) 2.0,38while, in hexane, I372/I385) 0.6.38Therefore, the CMT, which is the threshold temperature of self-aggregate formation by intra- and/or intermolecular association, could be determined from the change of the I372/I385ratio of pyrene in the presence of polymeric amphiphiles.37Figure 4 shows that the I372/I385ratio in an aqueous suspension of the F127-MNPs varies with temperature between the transition temperatures of 20 and 25 °C, which was the CMT of the F127-MNPs. The I372/I385ratio was higher in water below the CMT, indicating a strongly polar environment. However, above the CMT, the I372/
I385ratio dropped to a lower level, as the pyrene partition changed to a more hydrophobic environment as micellar aggregation began to form. These results were comparable with the CMT of pure F127 (23°C) in the literature,22,23which meant that the F127-MNPs was more hydrophobic above 25°C.
Another approach was based on the change of particle size of the F127-MNPs, with respect to temperatures, to indicate the hydrophilicity of the nanoparticles. As shown in Figure 4, the particle size of the F127-MNPs was 40.1 nm at 4°C and 37.8 nm at 15°C, but it sharply decreased to 19.3 nm at 25°C and 16.2 nm at 35°C, as measured by a DLS instrument (Zetasizer-3000HS, Malvern, U.K.). The particles exhibited a 2- and 2.3-fold diameter transition from 15 to 25°C and 35°C, respectively. That was roughly equal to a 10-fold volume transition from 15 to 35°C. The 10-fold volume shrinkage of the F127-MNPs was enough to pump the drug out.
3.3. Drug Delivery Test by HFMF. Figure 5a shows the results of inductive heating of the F127 MNPs, where the temperature was measured by an ethanol thermometer in an (32) Long, J. W.; Logan, M. S.; Rhodes, C. P.; Carpenter, E. E.; Stroud, R. M.;
Rolison, D. R. J. Am. Chem. Soc. 2004, 126, 16879–16889.
(33) Docoslis, A.; Huszarik, K. L.; Papageorgiou, G. Z.; Bikiaris, D.; Stergiou, A.; Georgarakis, E. AAPS J. 2007, 9, E361–E370.
(34) Hendra, P. J.; Agbenyega, J. K. The Raman Spectra of Polymers; John Wiley & Sons: New York, 1993.
(35) Moulder, J. F.; Stickle, W. F.; Sobol, P. E.; Bomben, K. D. A Reference
Book of Standard Spectra for Identification and Interpretation of XPS Data;
Physical Electronics, Inc.: Chanhassen, MN, 1995.
(36) Anderson, D.; Nguyen, T.; Lai, P. K.; Amiji, M. J. Appl. Polym. Sci.
2001, 80, 1274–1284.
(37) Kalyanasundaram, K.; Thomas, J. K. J. Am. Chem. Soc. 1977, 99, 2039– 2044.
(38) Wang, Y. S.; Liu, L. R.; Jiang, Q.; Zhang, Q. Q. Eur. Polym. J. 2007,
43, 43–51.
Figure 4.Hydrophilic/Hydrophobic test of F127-MNPs with various temperatures: filled circle curve indicates CMT test by PL (left axis), whereas particle size test by DLS (right axis) is indicated by open circle curve.
aqueous F127-MNPs suspension. Inductive heating is thermal energy induced from the hysteresis loss of ferrites and dependent on the type of remagnetization process in the HFMF.11The results showed that, under the selected field parameters (50-100 kHz and 15 kW), sufficient energy deposition was achieved, and the temperature was substantially increased in the solution within a short period of time. As expected, the temperature increased considerably (62 °C) for the F127-MNPs suspension (0.2 g samples in 10 mL of PBS in the tube) and was approximately 2.0 times higher than that of the pure F127 nanospheres (30°C), indicating that this temperature difference (62°C to 30°C,∆T ) 32°C) was solely attributed to the inductive heating effect of the iron oxide in the presence of HFMF.
Figure 5b shows the relationship between the temperature change and drug release behavior of the F127-MNPs. In the absence of the magnetic field, the drug (DOX) displayed a stable release at a rate of 0.23µg mL-1hr-1. However, while reaching 35°C under magnetic stimulus, the drug release rate increased sharply from 0.23 to 7.94µg mL-1hr-1during the first 5-min period (S-T1) and then reduced to 2.23µg mL-1hr-1 after a further 25-min stimulus (S-T2). The increased release rate when the temperature increased from 15 to 35°C (above the CMT) may be attributed to the volume shrinkage of the F127 shell layer. Similar reports have also been addressed in the literature.39 For instance, Chung et al. indicated that the PNIPAAm and
poly(butyl-methacrylate) polymeric micelles showed reversible structural changes, allowing drug release upon heating/cooling fluctuations with the LCST. These micelles released drug upon heating above the LCST, and the release was accelerated by a volume-shrinkage mechanism, like a pumping effect. The effect was eliminated upon cooling below the LCST.
Furthermore, upon magnetic manipulation, the drug also showed a two-stage release behavior. DOX exhibited a burst-like release for the first 5 min at a rate of ca. 38.77µg mL-1hr-1 (S-H1) and then stabilized to ca. 1.84µg mL-1hr-1(S-H2) for the following 25 min of operation. The rate of burst release in the first 5-min period with HFMF was 4.9 times higher than that at 35°C in the water bath. The plausible reason was due not only to the volume shrinkage at higher temperature but also to the change in the pore structure of the nanospheres under HFMF. Lu et al.4reported on ferromagnetic cobalt nanoparticles coated with gold shells (Co@Au nanopaticles) embedded into poly-electrolyte capsules. They demonstrated that such magnetic capsules resulted in an increase of wall permeability due to magnetostatic interaction between nanoparticles under oscillating magnetic field. Moreover, a similar mechanism of pore size enlargement under HFMF was also verified by BET analysis in our pervious work.13,16
The average pore diameter of the F127-MNPs was determined to be 7.2 and 11.6 nm without and with 10 min of exposure to the HFMF, respectively, as shown in Figure 6. The pore size after HFMF treatment was approximately twice that without HFMF treatment, and the pore was enlarged and even broken with HFMF treatment. This indicates that the nanostructure of the F127-MNPs can be manipulated with the HFMF and that the corresponding pore enlargement will induce a rapid drug release, i.e., a burst-like drug release pattern.
The inset TEM image of Figure 6 depicts the collapsed and cracked F127-MNPs. This suggests that the instantaneous drug release under HFMF was due not only to the volume shrinkage but also to the pore rupture of the structure. The collapsed situation was caused by a temperature increase due to generated heat, but the pore rupture might be induced by the violent magnetic vibration of nanoparticles under HFMF.15,16Therefore, HFMF-induced energy can cause the vibration of iron oxide and enlarge pores increasing the permeability of the F127.4Also, the heat energy was conveyed to shrink the F127 hydrogel to pump the drug out. As a result, an instantaneous drug release was achieved using the F127-MNPs by combining the thermal and dynamic energy (vibration of iron oxide nanoparticles) to pump the drug out. Both factors (heat and enlarged pore size) will increase the permeability of the F127, and thus causing the rapid release of the DOX from the F127-MNPs.
(39) Chung, J. E.; Yokoyama, M.; Yamato, M.; Aoyagi, T.; Sakurai, Y.; Okan, T. J. Controlled Release 1999, 62, 115–127.
Figure 5.(a) Inductive heating experiments under HFMF treatment; filled circle curve and open circle curve indicate F127-MNPs and F127 nanospheres, respectively; temperature increased to 62°C for the F127-MNPs under HFMF treatment for 60 min, but, for F127 nanospheres, it reached only 30°C. (b) Drug delivery test of F127-MNPs. Filled circle curve indicates that the samples were first incubated at 15°C (water bath) for 50 min and then exposed to HFMF (magnetic-thermal effect). Open circle curve indicates that, after incubation at 15°C for 50 min, the samples were incubated at 35°C in a water bath (thermal effect, without HFMF), but the open triangle curve means that the samples were incubated at 15°C in a water bath (50 + 30 min).
Figure 6.BET analysis on pore size change and TEM images of F127-MNPs with and without HFMF. One sample is without HFMF treatment (left side), and the other one is “after” the magnetic filed treatment (right side) in the TEM images.
effect and a rapid release of the anticancer drug upon short exposure to the HFMF offer a dual-functional therapeutic advantage for biomedical application. However, it would be better
quantum dots) for magnetic imaging or tracking. LA801451V