Hongbo
Wang‡
,
Jianhai
Yang‡
,
Yongmao
Li
,
Liang
Sun
and
Wenguang
Liu
*
School of Materials Science and Engineering, Tianjin Key Laboratory of Composite and Functional Materials, Tianjin University, Tianjin 300072, PR China. E-mail: wgliu@tju.edu.cn
First published on 24th October 2012
Monodisperse magnetic nanoparticles (MNPs) were prepared through an organic phase process, and the obtained MNPs were capped with poly[2-(2-methoxyethoxy)ethyl methacrylate]-b-poly[2-(dimethylamino)ethyl methacrylate] synthesized by surface-initiated atom transfer radical polymerization (ATRP). The MNPs-polymer brushes exhibited both superparamagnetic and thermoresponsive behaviors, and could condense plasmid DNA into nanocomplexes with a size of 100–120 nm at appropriate complexing ratios. Enhanced gene expression in COS-7 cells and HepG-2 cells was achieved under a magnetic field and variable temperature conditions due to magnetic force-facilitated internalization of nanocomplexes, and temporary cooling-triggered intracellular gene unpacking. Amazingly, combining magnetic field and temperature dual stimuli contributed to a 50–100- and 25–45-fold increase of the transfection efficiency in HepG-2 cells compared to conventional protocol and PEI25k, respectively.
In order to tune DNA unpacking, our group and other researchers have designed stimuli-responsive polymer vectors which were capable of responding to microenvironmental changes such as temperature, pH, light and redox by varying the macromolecular conformation.18–22 This self-adaptation attribute of smart polymers offers a promising way to address the dilemma of tight packing and dissociation of DNA in one single vector. Among the stimuli-sensitive nonviral vectors, thermoresponsive systems have been shown to improve gene transfection in a variable temperature mode due to temporary cooling-induced unpacking of genes from the carriers.23 However, all the thermoresponsive vectors developed thus far have only exhibited a modest level of transfection enhancement.23–28 Although several important parameters, including variable culture temperature timing, cationic character, hydrophobicity and lower critical solution temperature (LCST) range, have been optimized, the improvement of gene transfection is still marginal. A possible reason is that the low cellular uptake of nanocomplexes is the limitation to further improvement in the transfection efficiency of thermoresponsive vectors. In light of the advantages of magnetic field-induced increased internalization and temperature-tunable gene unpacking, we hypothesize that a nonviral vector integrated with temperature and magnetic responsive functions will demonstrate much higher transfection efficiency.
In this work, we prepared monodisperse magnetic nanoparticles (MNPs) through an organic phase process, and modified the MNPs with poly[2-(2-methoxyethoxy)ethyl methacrylate]-b-poly[2-(dimethylamino)ethyl methacrylate] diblock copolymer brushes which were formed via surface-initiated atomic transfer radical polymerization. The physicochemical properties of the MNPs-polymer brushes/DNA nanocomplexes were investigated and in vitro gene transfection of the MNPs-polymer brushes in COS-7 and HepG-2 cells under a magnetic field and variable temperature conditions were focused on.
:
1 v/v, pH adjusted with acetic acid), then with a water–alcohol mixture (1
:
1 v/v), with ethyl ether and finally dried under vacuum at room temperature overnight.
:
1 (DMAEMA/MNPs@Br) and at a weight ratio of 50
:
50
:
1(DMAEMA/MEO2MA/MNPs@Br), respectively.
The morphology and size of the MNPs@PMEO2MA50-PDMAEMA/pDNA complexes at the selected weight ratios corresponding to the maximum transfection efficiency were observed by JEOL JEM-100CXII TEM. Briefly, a drop of the complex solution was transferred onto a carbon-coated grid for 5 min and stained with 1.5 wt% phosphotungstic acid. Then the complexes were recorded on films with TEM. The particle size was estimated from the measurement of tens of particles found in a few randomly chosen areas in the TEM images.
After supplying complexes, the four groups of plates were first incubated for 2 h at 37 °C in 5% CO2. Subsequently, the magnets were removed, and the complexes that were not internalized were pipetted out and replaced with fresh medium. Group I and Group II were further incubated at a constant 37 °C for 46 h. For Group III and Group IV, after incubating at 37 °C for another 19 h, the plates were placed in a biochemical incubator for 3 h at 20 °C without changing any other conditions. Then the transfected cells were reincubated at 37 °C for an additional 24 h. After incubation, the culture medium was removed and the cells were washed with PBS twice. The cells in each well were treated for 15 min with 150 μL of reporter lysis buffer (RLB, Promega), followed by freeze–thaw cycles to ensure complete lysis. The lysate was centrifuged for 3 min at 13
000 rpm and the supernatant was collected for luminescence measurements. The luminescence of each sample was measured by a 1420 Multilabel counter (Wallac, USA) using the Bright-GloTM luciferase assay system (Promega, USA) according to the manufacturer's protocol. The results were expressed as relative light units (RLU) per milligram of cell protein, and the protein concentration of each well was measured by a BCA protein assay (Pierce, Rockford, IL, USA). 25 kDa branched polyethylenimine (PEI25k) served as a positive control. A PEI25k/pDNA complex with weight ratio of 2
:
1 was prepared as the reported protocol.19
:
1 served as a control.
:
1 to 40
:
1 were added into each well and incubated for 24 h before refreshing the medium with fresh complete medium (200 μL per well). After incubation for another 24 h, 20 μL per well MTT (5 mg mL−1 in PBS) was added to each well, and the plate was further incubated for 4 h. Then, all media were removed and 150 μL per well DMSO was added, followed by shaking for 30 min. The absorbance of each well was measured at 570 nm on a ∑960 plate-reader (Metertech) with pure DMSO as a blank. Non-treated cells (in DMEM) were used as a control and the relative cell viability (mean% ± SD, n = 3) was expressed as ODsample/ODcontrol × 100%.
![]() | ||
| Scheme 1 Synthetic procedure for MNPs@PMEO2MA-PDMAEMA. | ||
High resolution transmission electron microscopy (HRTEM) images of MNPs are exhibited in Fig. 1. The crystal structure of the MNP phase can be clearly seen in the photograph (A). The diameter of the MNPs is mainly around 4 nm. In Fig. 1B, one can easily distinguish the polymer brush layer from the MNP cores, because of the different contrast between the amorphous polymer phase and the crystals.
![]() | ||
| Fig. 1 HRTEM photos of MNPs (A) and MNPs@PMEO2MA50-PDMAEMA150 (B). (C and D): TEM image of MNPs taken with a 10 nm scale bar and size distribution. | ||
The magnetization curves of the as-synthesized nanoparticles and polymer-grafted MNPs were tested at 300 K (Fig 1S†). As shown in the figure, the saturation magnetization values of the OA-modified MNPs and MNPs-polymer brushes are about 20.1 emu g−1 and 16.8 emu g−1, respectively. It is evident that capping the MNPs with polymer lowers the magnetization to a certain degree. Importantly, neither coercivity nor remanence is observed in the magnetization curves, indicating the superparamagnetic behavior of the MNPs.
Fig. 2S† shows the FTIR spectra of the samples. The featured absorption bands of DMAEMA are located at 1730 cm−1 (C
O), 1148 cm−1 (C–O) and 1456 cm−1 (C–N).33 It is noted that the main characteristic peaks of MEO2MA overlap with those of DMAEMA. Nevertheless, the increased peak intensity of C–O (1148 cm−1) in the MNPs@PMEO2MA50-PDMAEMA150 compared to that in MNPs@PDMAEMA150 is evidence of the successful copolymerization of MEO2MA.34 To further verify if PMEO2MA was grafted onto the MNPs, the LCSTs of MNPs-polymer brushes solutions which reflect the thermoresponsive behavior were determined. Fig. 2 demonstrates that both MNPs@PMEO2MA50-PDMAEMA50 and MNPs@PMEO2MA50-PDMAEMA150 aqueous solutions exhibit their LCSTs at around 31 °C and 33 °C, respectively, suggesting the existence of PMEO2MA segments. The higher LCST of MNPs@PMEO2MA50-PDMAEMA150 is due to the enhanced hydrophilicity of the copolymer with longer chains of PDMAMEA.
![]() | ||
| Fig. 2 Light transmission versus temperature curves of MNPs@PDMAEMA, MNPs@PMEO2MA50-PDMAEMA50 and MNPs@PMEO2MA50-PDMAEMA150 in PBS solution (pH = 7.4, 0.5 wt%). | ||
Fig. 3S† displays the TGA curves of the MNPs modified with PDMAEMA and PMEO2MA-PDMAEMA. We note that the MNPs@Br has only a little mass loss from room temperature to 600 °C (not shown), which is ascribed to the thermal decomposition of initiator molecules. In contrast, the remaining masses (%) of MNPs@PDMAEMA150 and MNPs@PMEO2MA50-PDMAEMA150 are between 0 and that of MNPs@Br, due to grafting different polymer contents. Based on the data from TGA, the polymer contents in MNPs@PDMAEMA150 and MNPs@PMEO2MA50-PDMAEMA150 are calculated to be 94.14% and 85.99%, respectively. The lower content of copolymer in the hybrid nanoparticles may be attributed to the steric hindrance of the first segment of PMEO2MA, which affects the polymerization of DMAEMA.
:
1 and 1
:
1, respectively. The condensation ability of MNPs@PMEO2MA50-PDMAEMA50 is apparently inferior to that of MNPs@PMEO2MA50-PDMAEMA150 due to shorter polycationic segments. The poorer DNA condensation ability may affect the transfection efficiency. Therefore, in the following tests, we only characterized the physicochemical properties of MNPs@PMEO2MA50-PDMAEMA150, and focused on its gene transfection driven by magnetic field and temperature.
![]() | ||
| Fig. 3 Agarose gel electrophoresis patterns of MNPs@PMEO2MA50-PDMAEMA50/pDNA complexes (A) and MNPs@PMEO2MA50-PDMAEMA150/pDNA complexes (B) at varied weight ratios. | ||
The hydrodynamic sizes of the MNPs@PMEO2MA50-PDMAEMA150/DNA complexes at varied ratios were measured and the results are shown in Fig. 4A. The average diameters exhibit a declining trend with increments in complexing ratio. While the ratio is above 10
:
1, the sizes drop to less than 120 nm, which is roughly consistent with the results obtained from the TEM images shown in Fig. 5. The particle size in this range can readily undergo endocytosis.31Fig. 4B displays the zeta potentials of the MNPs@PMEO2MA50-PDMAEM150/pDNA complexes determined at various ratios. Clearly, the zeta potentials show a rising trend with increasing ratio up to 14, and then level off at higher ratios. The appropriate positive surface charge density of the MNPs@polymer brushes enables tighter packing of DNA, resulting in much smaller complexes at a higher complex ratio, which will increase the affinity of complexes to negatively charged cell membrane surfaces, thereby facilitating the cellular uptake of nanoplexes.35
![]() | ||
| Fig. 4 Hydrodynamic diameters (A) and zeta potentials (B) of MNPs@PMEO2MA50-PDMAEMA150/pDNA complexes at different weight ratios. | ||
![]() | ||
Fig. 5 TEM images of negatively stained vector/pDNA complexes: MNPs@PMEO2MA50-PDMAEMA150/pDNA at 10 : 1 (A), MNPs@PMEO2MA50-PDMAEMA150/pDNA at 12 : 1 (B), MNPs@PMEO2MA50-PDMAEMA150/pDNA at 20 : 1 (C) and MNPs@PMEO2MA50-PDMAEMA150/pDNA at 24 : 1 (D). | ||
:
1 to 16
:
1(Fig. 6 and 7). The thermal gravimetric analysis (Fig. S3†) indicates that the content of magnetic nanoparticles (MNPs) in the hybrids is lower than those obtained by traditional methods, and the MNPs-polymer brushes are well dispersed in aqueous solution. So, while magnetic field was applied, it took a longer time for the MNPs to settle down. In our experiment, we found that a treatment duration shorter than 2 h could not lead to satisfactory cellular internalization. In addition, it is necessary to point out that we observed no aggregation of the MNPs-polymer/DNA complexes in serum during transfection.
![]() | ||
| Fig. 6 In vitro gene transfection efficiency of the MNPs@PMEO2MA50-PDMAEMA150/pDNA complexes in comparison with that of PEI25k at various weight complexing ratios in COS-7 cells cultured in the DMEM containing 10% FBS. Non-M: without a magnetic field; M: magnetic field; VT: variable temperature; CT: constant temperature. Results are presented as the mean ± SD in triplicate. The same letters labeled in the figure indicate there is no significant difference; different letters indicate significant difference among the experimental groups. P < 0.05. | ||
![]() | ||
| Fig. 7 In vitro gene transfection efficiency of the MNPs@PMEO2MA50-PDMAEMA150/pDNA complexes in comparison with that of PEI25k at various weight complexing ratios in HepG-2 cells cultured in the DMEM containing 10% FBS. Non-M: without a magnetic field; M: magnetic field; VT: variable temperature; CT: constant temperature. Results are presented as the mean ± SD in triplicate. The same letters labeled in the figure indicate there is no significant difference; different letters indicate significant difference among the experimental groups. P < 0.05. | ||
Fig. 6 clearly shows that combined application of a magnetic field and temporary cooling achieves a higher transfection level than the other three routes of constant temperature without applying a magnet, constant temperature with applying the magnet and variable temperature without the magnet in COS-7 cells. At a 10
:
1 ratio, under magnetic and temperature dual stimuli, the MNPs-polymer brushes achieve the highest efficiency, 3.46 × 108 RLU per mg protein, which is 4-fold higher than that of normal culture conditions and comparable to that of PEI25k. The decrease of transfection efficiency at higher complexing ratios may result from the cytotoxicity of the vector.
Amazingly, the transfection efficiencies of the MNPs-polymer brushes in HepG-2 cells are significantly increased under magnetic field and temperature stimuli compared to the other three protocols (Fig. 7). The transfection level of the complexes with either application of a magnet or cooling treatment is about 15-fold higher than that of constant temperature without the magnet at the optimum ratio. The transfection efficiency with both magnetic field and temperature stimuli is about 10–20 and 50–100 times more than that of either applying a magnetic field or cooling treatment and constant temperature without a magnetic field, respectively, at the selected ratios. Dual stimuli also result in 25–45 times better efficiency than PEI25k. We note that for temperature insensitive PEI25k, there is no significant difference in the transfection efficiencies in Non-M/VT and Non-M/CT modes. Thus, it is rational to think that the increased transfection level under variable temperature conditions is mainly from the thermoresponsive behavior of the MNPs-polymer brushes.
To further evaluate the gene transfection of the MNPs-polymer brushes by the four protocols, we assessed the expression of pEGFP in HepG-2 cells at an optimum weight ratio. GFP expression was analyzed by flow cytometry (Fig. 8). It can be seen that both MNPs@polymer brushes and PEI25k achieve efficient GFP expression. Comparatively, the MNPs-polymer brushes are more potent than PEI25k in mediating GFP expression in the four methods. The transfection efficiency obtained under a magnetic field or at variable temperature conditions is around 19%, more than twice that of PEI25k. Similarly, combining magnetic field and temperature stimuli leads to more prominent gene expression than any single stimulus. 29.35% of cells express GFP, 3 times higher than that of PEI25k.
![]() | ||
Fig. 8 Analysis results of GFP expression mediated by MNPs@PMEO2MA50-PDMAEMA150/pDNA in HepG-2 cells using a flow cytometer. Control: naked DNA; PEI25k/pDNA(2 : 1, wt/wt); MNPs@PMEO2MA50-PDMAEMA150/pDNA(12 : 1, wt/wt) at different conditions. | ||
The considerable improvement in transfection efficiency under magnetic field and temperature stimuli is due to the increased internalization of nanocomplexes, as well as efficient gene unpacking in cytoplasm. The magnetic field-generated attractive force can facilitate the rapid sedimentation of complexes on the surface of cell membranes and pull the magnetic vector/DNA nanoparticle across the barrier of the plasma membrane. As a result, more nucleic acids are ferried into the cells. This can be confirmed by the results of flow cytometry (Fig. 9). As shown in the figure, both the internalization rates of PEI25k and the MNPs@polymer brushes are more than 96%. But the average fluorescence intensity is significantly different, in that the intensity of the MNPs@polymer brushes/DNA complexes in the presence of a magnetic field is 1.9-fold that in the absence of a magnet, and 6-fold that of PEI25k. After magnetic field-driven increased entry of nanocomplexes into the cells, temporary cooling leads to the hydration of poly[2-(2-methoxyethoxy)ethyl methacrylate] chains from dehydrated collapse, which contributes to more exposure of genes for transcription.36 Thus, the synergistic effects of magnetic field and temperature stimuli achieve much higher gene transfection levels. The mechanism of the magnetic field/temperature stimuli-induced enhancement in gene transfection is depicted in Scheme 2. In previous work,36,37 a variable temperature approach was reported to lead to several times improvement in gene expression compared to conventional transfection. In this study, a 50–100-fold increase in transfection was accomplished with combined application of a magnetic field and temperature.
![]() | ||
Fig. 9 Cellular internalization of complexes at a weight ratio of 12 : 1 by HepG-2 cells in the presence and absence of a magnetic field. | ||
![]() | ||
| Scheme 2 The mechanism of the magnetic field/temperature stimuli-induced enhancement in gene transfection. | ||
:
1 to 16
:
1, more than 80% of cells remain viable. At 40
:
1, the cell viability decreases to 66%. Taken together, we have shown that the MNPs-polymer brushes/pDNA complexes are less cytotoxic than PEI25k over the best transfection complex ratios.
Footnotes |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c2tb00203e |
| ‡ Equal contribution. |
| This journal is © The Royal Society of Chemistry 2013 |