Chao-Fan Dai†
a,
Wei-Yuan Wang†a,
Lin -Wanga,
Lei -Zhoua,
Shu-Ping Li*ab and
Xiao-Dong Li*a
aJiangsu Key Laboratory of Biofunctional Material, College of Chemistry and Material Science, Nanjing Normal University, Nanjing, 210023, China. E-mail: lishuping@njnu.edu.cn; Fax: +86 25 83598678; Tel: +86 25 83598280
bJiangsu Provincial Key Laboratory of Palygorskite Science and Applied Technology, Huaiyin Institute of Technology, Huaian, 223003, P. R. China
First published on 12th July 2016
Biomedical applications of nontoxic amorphous calcium carbonate (ACC) have mainly been restricted because of its aqueous instability. Herein, we report the successful synthesis of highly stable ACC–methotrexate (MTX)@SiO2 nanospheres in vitro for use in cancer therapy. Further, vaterite–MTX@SiO2 nanospheres were also prepared for comparison. In our synthesis procedure, ACC–MTX and vaterite–MTX were firstly prepared at different pH values, and then SiO2 layers were subsequently deposited by the well-known Stöber method. The results indicated that the special structure of ACC–MTX@SiO2 presents better controlled-release and results in efficient death of cancer cells, thus showing its great potential as a desirable chemotherapeutic system for cancer therapy.
In this paper, nanosized ACC-drug and vaterite (a kind of crystallized CaCO3)-drug hybrids were firstly synthesized, and then a silica-based core–shell structure was introduced to improve the stability. Typically, this kind of system usually consists of a CaCO3-drug core and a permeable shell, and the permeable shell should protect the core from unexpected drug leakage. Such similar structure of ACC–DOX@SiO2 was also prepared by Zhao group, however the aqueous instability still restricted its further utilization.8 Herein, methotrexate (MTX), which can effectively deactivate the metabolism of diseased cells through programmed cell death or apoptosis, was chosen as the anticancer drug. More importantly, the formation mechanism and anticancer effect was explored emphatically.
Here, a possible mechanism was proposed for the formation and growth of CaCO3–MTX@SiO2 structure, as illustrated in Fig. 1e. Firstly, MTX molecules were bound or chelated with Ca2+ to form Ca2+–MTX structure.10 Secondly, the obtained Ca2+–MTX would react with CO32− anions to form CaCO3–MTX NPs. Finally, the obtained CaCO3–MTX NPs were subsequently coated with SiO2 by the well known Stöber method, and then CaCO3–MTX@SiO2 was formed.
Further, these four samples were also characterized by XRD and IR. For XRD analysis, ACC–MTX exhibited no distinct diffraction peaks, and two typical broad lumps at 2θ angle of approximately 30° and 45° represented the formation of ACC.11 On the contrary, vaterite–MTX fitted well with the International Centre for Diffraction Data (ICDD) database of PDF#72-0506, confirming the existence of vaterite. What's more, the weak reflection plane at about 23° for samples b and d (Fig. 1f) belonged to the diffraction pattern of the silica layer. The corresponding Fourier transform infrared (FTIR) spectra were also exhibited in Fig. 1g. For all samples, the bands at 1460, 1090 and 877 cm−1 were due to the ν3 asymmetric vibration, ν1 symmetric and ν2 asymmetric vibration of CO32−, respectively.12,13 As for vaterite–MTX hybrid, the formation of vaterite was confirmed by the presence of ν4 symmetric vibration at 746 cm−1, which is characteristic of crystalline calcium carbonate (vaterite) phase only.14 In addition, the peak centered at 1095 cm−1 belonged to the deformation mode of Si–O–Si, which appeared in both ACC–MTX@SiO2 and vaterite–MTX@SiO2.
In vitro release profiles of four samples had been illustrated in Fig. 2A, which obtained in phosphate buffer saline (PBS) of pH = 7.4. A rapid release of MTX occurred at the initial stage, which followed by a relatively slower one. Such two-step and prolonged release behavior could benefit the therapeutic treatment, as the initial release rapidly provided a therapeutic dose, and the subsequent sustained release allowed maintenance of this dose over a long period of time.15 In details, the t0.5 (the time for release fraction of 50%) is 10 min, 4 h, 30 min, 7 h for samples a, b, c and d, respectively. The burst release fractions (defined as the release fraction in the initial 5 h) are 69%, 54%, 59% and 50%, respectively. It is obvious that silica-coated particles present much better controlled-release property than those of non-coating ones. We think that core–shell structure might experience two-step of the drug-release process, and the first one is that MTX dissociates from the CaCO3–MTX complex by an acid-induced decomposition of the core. The second one is that MTX passes through the silica shell and enters into the external environment. Consequently, the silica-coating structure exhibited much better controlled-release than that of CaCO3–MTX NPs.
There are about two kinds of mechanism on the drug release, i.e., ion-exchange process and dissolution of outer layers in buffer solution, and the release process could be controlled by any of the steps. To gain more insights into the mechanism of drug release, four types of kinetics models were exploited:16 the Higuchi model (eqn (1)), the Bhaskar equation (eqn (2)) and the Ritger–Peppas equation (eqn (3)) and parabolic diffusion equation (eqn (4)):
Mt/M∞ = kHt0.5 | (1) |
lg(1 − Mt/M∞) = −kBt0.65 | (2) |
Mt/M∞ = ktn | (3) |
(Mt/M∞)/t = kPt−0.5 + b | (4) |
In the above equations, Mt/M∞, t, k are the fractional drug release, release time and the corresponding release rate constant, respectively, and a and b are constants whose chemical significance is not clearly resolved.
On the basis of the four different kinetic models, the fitting results of drug release profiles are given in Fig. 2B, and the corresponding linear correlation coefficients (R) and n values obtained from the fittings are summarized in Table 1. It can be seen from Fig. 2B and Table 1, the Higuchi and the Bhaskar equation are not suitable to explain the release process reflected by the fact that modeling data points do not form a straight line and small linear correlation coefficients (R < 0.96). As for samples a and c, parabolic diffusion model fits the release data much better (R > 0.98). While for samples b and d, the fitting coefficients of Ritger–Peppas model are the highest (R > 0.98). Usually, the R–P equation (eqn (3)) used to explain drug diffusion and dissolution of layers. The value of n < 0.45 corresponds to the drug diffusion control, which based on ion exchange process; n > 0.89 is attributed to the dissolution of layers; 0.45 < n < 0.89 is due to the cooperation of drug diffusion and layer dissolution. The parabolic diffusion equation (eqn (4)) elucidates that the release process is controlled by an external surface/edge diffusion process.17,18 For samples a and c, they can be described by external surface diffusion as the rate-controlling step, and MTX anions are diffused into the medium solution from the surface of CaCO3 particles, owning a rapid drug release process. Whereas, the release process of samples b and d, with release value of n between 0.1861 and 0.2265 (n < 0.45), belongs to the drug diffusion via ion exchange, based on the MTX anions diffusion from the interlayer CaCO3 core to the surface of particles, which takes a rather longer release time.
Samples | Higuchi | Bhaskar | Ritger–Peppas | Parabolic diffusion | |
---|---|---|---|---|---|
R | R | R | n | R | |
a | 0.823 | 0.831 | 0.972 | 0.177 | 0.980 |
b | 0.842 | 0.864 | 0.981 | 0.070 | 0.961 |
c | 0.918 | 0.912 | 0.971 | 0.061 | 0.981 |
d | 0.842 | 0.856 | 0.982 | 0.054 | 0.958 |
The cell cytotoxicity and anticancer efficiency of samples a–d together with MTX are evaluated by bioassay test. Firstly, the cytotoxicity evaluation of samples a–d and MTX was carried out on both normal (PC-12) and cancer cell (A549) lines, and cell viability was evaluated at a concentration of 100 μg mL−1 after 24 h of incubation (in Fig. 3K and L). As displayed in Fig. 3K, ACC–MTX and ACC–MTX@silica had little toxic effect on normal cells, while vaterite–MTX and vaterite–MTX@silica were fairly toxic and block viability of the cells obviously.19,20 As expected, MTX was fairly toxic on normal cells. However, as for cancer cells of A549 (Fig. 3L), MTX showed little effect on them. From Fig. 3L, silica-coating nanoparticles exhibited enhanced anticancer effect compared with those of non-coating ones, especially after long-time incubation. In details, the cell viability of ACC–MTX, vaterite–MTX and MTX did not change much with the increase of time. However, the cell viability of vaterite–MTX@silica and ACC–MTX@silica showed a rapid decrease as the extension of time, probably due to the enhanced controlled-release effect after silica coating. Considered from the above results, the formation of ACC–MTX@silica structure not only can decrease the side effects on normal cells but also enhance the anticancer effect on the meanwhile, showing a kind of potential treatment candidate for cancer therapy. Furthermore, a contrast study on cancer and non-cancerous cells from Fig. 3K and L demonstrated that samples a–d have obvious suppression effect on cancer cells than normal cells.
As a supplement to MTT assay, morphology changes of A549 cells treated with DMEM, pure MTX (100 μg mL−1), samples a–d (100 μg mL−1) after 72 h of incubation were displayed in Fig. 3A–F. The cells treated with DMEM showed normal cellular morphology of A549, indicating that living cells look like spindles (Fig. 3A). The cell form was slightly changed after treated with MTX, and the co-existence of spindle and circular cells mean that part of A549 cells were withered or close to death after the uptake of MTX (Fig. 3B). As expected, addition of samples a and c had noticeable effect on A549 cells, revealed by lots of circular cells, displaying that most of A549 cells died (Fig. 3C). Notably, it was worthy to reveal that almost all cells treated with samples b and d exhibited circle in morphology, presenting that almost all cells underwent apoptosis (Fig. 3D). In order to further explore the uptake process of ACC–MTX@silica nanostructure into A549 cells, the intracellular location observed by phase contrast images were also carried out at different incubation time for sample d (see Fig. 3G–J). The results demonstrated that cells morphology changed dramatically with the incubation time. After 0.5 h of incubation, the cells became slightly shrank and a small amount of NPs accumulated at the nearby of cell membrane (Fig. 3H). When the duration increased to 1 h, most of particles were internalized into the cytoplasm, such rapid amassing also suggested a distinct mechanism, i.e., the endocytosis effect may be involved in the uptake of ACC–MTX@silica.21 At the same time, cell morphology became irregular (Fig. 3I). After 2 h of incubation, ACC–MTX@silica nanoparticles still laid free in the cytoplasm, but the cells shrank into an ellipse (Fig. 3J). For comparisons, the intracellular location of A549 cells without adding any drug was also shown in Fig. 3G. The distinct morphology changes presented that the core–shell structure of ACC–MTX@silica is a kind of promising treatment platform for cancer therapy.
Footnote |
† These authors contributed equally to the work. |
This journal is © The Royal Society of Chemistry 2016 |