Bogdan V. Parakhonskiy‡*ab,
Cristina Foss‡ac,
Eleonora Carlettiac,
Mariangela Fedelac,
Albrecht Haased,
Antonella Mottaac,
Claudio Migliaresiac and
Renzo Antolinid
aBIOtech Research Center, Department of Industrial Engineering, University of Trento, via delle Regole 101, 38123 Mattarello, Italy. E-mail: bogdan.parakhonskiy@gmail; Fax: +39 0461 883659; Tel: +39 0461 882774
bShubnikov Institute of Crystallography, Russian Academy of Science, Leninskii prospekt 59, Moscow 119333, Russia
cINSTM-Consorzio Interuniversitario Nazionale per la Scienza e Tecnologia dei Materiali, via G. Giusti 9, 50121 Florence, Italy
dDepartment of Physics, University of Trento, via Sommarive 14, 38123 Povo, Italy
First published on 13th August 2013
Porous vaterite containers of 400 nm size are studied with respect to intracellular drug delivery applications. A generic crystal phase transition from vaterite to calcite serves as a novel payload release mechanism, which reveals a delayed burst-release. This will permit control of the pharmacokinetics allowing for applications like preventive drug administration or scheduled application of pharmaceuticals during long term therapy. Experiments with two types of payloads, providing different molecular weights and zeta-potentials, demonstrate a flexible way of tailoring the payload delivery time via the molecular properties of the cargo. A dual in vitro cellular uptake experiment with human ovarian carcinoma cells ES2 and human fibroblasts MRC5 shows no cytotoxicity, no influence on cell viability, and fast penetration of substance-loaded containers into cells. Flow cytometry analysis proves high uptake rates and 3D microscopy analysis reveals the intracellular distribution.
Porous calcium carbonate in the form of polycrystalline vaterite spheres is one of the most promising systems in this respect.6,27 For micrometer-sized vaterite particles many favourable properties have already been demonstrated, such as biocompatibility, high drug-loading capacity, and payload protection.6,14,16,18 However, only recently these particles could be successfully scaled down to sub-micron sizes.28 This implies an enormous increase of the system's potential for drug delivery applications9,29,30 since the achieved mono-dispersed size distribution around 400 nm now allows accessing micrometer-sized cells or tissue structures.
After shrinking the size, an important issue is the investigation of the containers’ release dynamics and its controllability. The two most common processes exploited for cargo release from porous particles are desorption–adsorption6,10,11 and dissolution of the carriers.29 But both processes offer rather limited control of the release rate.10 However, realistic carrier systems for nanomedicine need control of the pharmacokinetics. Two common scenarios are predisposed for controllable delayed substance release: preventive intake when direct administration is inconvenient e.g. for symptoms that follow circadian rhythms like hypertension, ischemic heart disease, asthma, or rheumatoid arthritis;31 the other is a scheduled application during long term therapy e.g. of cancer,32 diabetes,33 ulcerative colitis,34 osteoporosis,35 or osteomyelitis.36
In the carrier system based on vaterite, proposed in this work, this temporal control can be realized by exploiting a novel feature of these particles in the sub-micron regime: the metastable carriers undergo a crystal phase transition from vaterite to calcite, during which the loaded substance is released almost completely. As recently shown, this mechanism allows a control of the payload delivery time via the properties of the particles and the environment.28 In this paper, first cellular uptake experiments of these sub-micron carriers are presented, their influence on cell vitality and metabolism is characterised, and a flexible way of tailoring the substance release dynamics via the payload molecular structure is demonstrated.
000×. Statistical image analysis was performed using ImageJ (NIH) based on n = 100 particles per sample.
For the preparation of sterile loaded particles, empty containers were stored in pure ethanol at 4 °C overnight. They were centrifuged at 3000 rpm for 4 min and immersed in a sterile dye solution as described before. The containers were subsequently suspended in sterile distilled water and centrifuged 3 times to remove residual ethanol and dye. Finally, containers were suspended in fresh medium at high (100 μg ml−1) or low (30 μg ml−1) concentration and used for cell incubation 24 h after seeding.
000 rpm, resuspended in PBS at a concentration of 1 × 106 cells per ml, and transferred to 5 ml tubes (BD Biosciences). Cell samples were then analysed using a Four-colour flow cytometer from FACSCalibur (Becton Dickinson). Forward and side scatter signals were analysed to identify cell populations. A background signal was obtained by measuring the autofluorescence of negative control samples containing unloaded cells. Cell samples with TD4-loaded particles were analysed by recording the signal in the FL-2 channel (ex. 488 nm, em. 585/42 nm), while the signal from Rh6G-loaded particles was recorded from the FL-1 channel (ex. 488 nm, em. 530/30 nm). Following instrumental optimization, the acquisition parameters (amplification and threshold) were kept constant throughout the whole experiment. For each sample 10
000 events were recorded. Data were analysed with the CellQuest Pro 6.0 software (Becton Dickinson), providing median intensity values and percentage of stained cells above a 98-percentile threshold of the control sample fluorescence distribution. Differences in cell populations were analysed with the Kolmogorov–Smirnoff test with a statistical significance of p ≤ 0.01.38
As proof-of-principle experiments, two fluorescent markers were loaded into the vaterite containers: Rhodamine 6G (Rh6G) with a low molecular weight of 480 Da and TRITC-dextran (TD4) where the attachment of the dextran group increases the molecular weight by one order of magnitude to 4.4 kDa. In this way, payload uptake and release could be studied by fluorescence microscopy and spectrofluorometry for payloads of different molecular properties.
For the high molecular weight cargo TD4, the loading efficiency was 157 ± 24 μg mg−1. For the low molecular weight substance Rh6G, the loading efficiency depended on the number of washings. One to four repetitions resulted in efficiencies from 8 ± 2 μg mg−1 to (7 ± 2) × 10−2 μg mg−1. These efficiencies are of the same order as those of other substances loaded via adsorption into porous carriers.39–41 Loading by coprecipitation might still allow us to increase these values,11 but quantification will be more demanding.
The surface properties of the loaded particles were characterised by zeta-potential measurements. Particles with TD4 cargo maintained a negative zeta-potential (changing from −11 mV to −25 mV), while the particles loaded with Rh6G changed to +4 mV.
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| Fig. 1 Particle recrystallization in media: (A) and (B) represent a scheme of the release mechanism and the corresponding 2PM fluorescence images from the containers, with SEM images as insets. In (A) the carriers are in a pure vaterite phase loaded with Rh6G; (B) shows the calcite phase where the dye was released to the medium apart from residuals attached to the crystal edges; (C) shows dye release curves for different payloads measured by spectrofluorometry during the immersion in water and in ethanol. | ||
The fluorescence images demonstrate a release of the dye during this recrystallization process, leaving the centres of the calcite monocrystals dark with residual dye attached only to their surfaces (Fig. 1B). The dye release curves are shown in Fig. 1C. In the case of particles with the low molecular weight cargo Rh6G immersed in water, after days 1 and 2, 25 ± 8% of the dye were found in the solution, which can be attributed to a desorption–adsorption process: the dye is slowly released until a dynamic equilibrium is obtained. After days 3 and 4, the recrystallization process speeded up the payload release, raising the amount of dye molecules in the solution to 40 ± 7%.
After the complete recrystallization of all vaterite spheres at day 5, up to 86 ± 13% of the initially loaded dye was detected in the solution. The residual dye remained attached to the calcite surface or within inter-particle gaps.
A BET analysis during the phase transition from vaterite to calcite resulted in a particle surface shrinking from 22 to 6 m2 g−1, owing to the transformation of porous spheres into rhombohedral monocrystals. The zeta-potential fell to 0 mV.
Immersion of the vaterite particles in ethanol showed only a slow release via adsorption–desorption (Fig. 1C). The total amount of released dye was found to be 22 ± 5% at day 1 and did not increase significantly until day 6. This manifests a desorption–adsorption equilibrium without crystal phase transition. A negative zeta-potential measured throughout the whole experiment emphasizes the stability of the containers.
For the particles loaded with the high molecular weight cargo TD4 instead, no recrystallization was observed in any of the media during the first week. During this time only a slow dye release (<10%) via desorption was found (Fig. 1C). In this case, the recrystallization process was completed only after 9 days. These dynamics can be explained by a strong attachment of TD4 to the vaterite surface. This manifested itself also by the stronger negative zeta-potential, which prevents container aggregation by electrostatic repulsion. Moreover, TD4 as a polymer decreases the rate of carrier dissolution,43,44 which consequently reduces the recrystallization and substance release rate with respect to lower weight cargos. These mechanisms open up the possibility to actively tune the release dynamics via the payload structure, such as the attachment of a dextran group to the fluorescent marker causing a retardation of the dye release.
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| Fig. 2 Cytotoxicity analysis of (A) Rh6G- and (B) TD4-loaded vaterite containers: the absorbance is proportional to the concentration of LDH, which in turn is directly dependent on cell death. ES2 cells were put in direct contact with vaterite particles at two concentrations: 100 μg ml−1 (High) and 30 μg ml−1 (Low) for 24 h. Alternatively, extracts from containers were added to culture media (Extracts). Fresh medium (no Caps) and pure PBS were used as negative controls. As a positive control, cells were cultured in a medium with 1 mM of Triton X-100. No significant differences could be detected between the samples and the negative control, while the absorbance of the positive control was significantly higher, indicating no cytotoxicity of the containers. | ||
Then, cell viability was monitored for 48 h of incubation with both concentrations of dye-loaded particles. The results are demonstrated in Fig. 3. The alamarBlue fluorescence signal is proportional to the number of viable cells in each sample at each time point. In all cultures a significant increase in cell viability was found after 24 h and 48 h of incubation regardless of cargo type or concentration. The number of viable cells in the samples in contact with dye-loaded particles at both concentrations showed no significant viability reduction with respect to the control samples without particles, indicating that the presence of the vaterite containers did not modify cell metabolism or viability.
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| Fig. 3 Cell viability measured at different times using an alamarBlue assay on ES2 cells incubated with 100 μg ml−1 (High) or 30 μg ml−1 (Low) of (A) Rh6G- and (B) TD4-loaded vaterite containers in culture medium. Cells cultured without particles were used as a control. The viability of cells in contact with containers shows no significant decrease with respect to the control samples at all times. | ||
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| Fig. 4 ES2 cells 48 h after adding the containers loaded with Rh6G (A, C) and TD4 (B, D). The green channel represents the calcein fluorescence labeling of the cells, and the red channel shows the fluorescent markers delivered by the containers. The figures comprise projection views onto 3D image stacks (A, B) and a zoom onto single cells comprehended by perpendicular sections along the crosslines (C, D), which proves a complete internalization of the carriers. All scale bars correspond to 10 μm. | ||
Both cell lines ES2 and MRC5 showed very similar results: containers of different payloads reveal different uptake dynamics. For Rh6G-loaded containers the fluorescence distributions demonstrate that the payload had entered the cells already after 2 h (Fig. S1 and S2†). The fluorescence signal from inside the cells increased significantly after 24 h and 48 h of incubation. This suggests a correlation between the uptake mechanism and metabolic activity, since the number of metabolically active cells increased strongly at the same time points in the viability tests.
TD4-loaded containers instead could not be detected within the cells after 2 h or 8 h and only with the increase of metabolic activity after 24 h, TD4 fluorescence inside the cells proved an uptake of the containers. These different uptake times can be explained again by the different payload properties: while loading the containers with TD4, their zeta-potential becomes more negative. Rh6G-loading instead shifts the zeta-potential into the positive (see Paragraph 2.1), which favours the cellular uptake due to an attraction to the negatively charged cell membrane.45
Fig. 4 shows ES2 cells after 48 h of incubation with dye-loaded containers. A complete internalization of the containers is proven by perpendicular image sections (Fig. 4C and D) which complement the projection views onto the cell layers.
Also the fluorescence distribution within the cells turned out to be very different for the two payloads. Fig. 4A and C show cells with Rh6G-loaded particles; the dye is distributed within the cell in a form that suggests a partial release from the carriers and subsequent staining of the mitochondria.46,47 The characteristic difference between the mitochondria morphology of fibroblasts and tumor cells is reflected by the fluorescence pattern showing rather elongated structures for the latter.48,49 This early release can be attributed to the desorption–adsorption process which was also observed in solution.
In the case of TD4-loaded containers instead (Fig. 4B and D), the shape and size of the fluorescent centres suggest that the dye is still confined in the vaterite spheres, which is in agreement with the release dynamics measurement in solution.
The cellular uptake of the containers was analysed also quantitatively via flow cytometry. Fig. 5 shows the result for ES2 cells after 24 h and 48 h of incubation. The three curves correspond to cells incubated in media with a high concentration of containers, with low concentration, and without containers. The upper figures show data for Rh6G loaded containers, the lower figures for TD4-loaded containers. The corresponding results for the MRC5 cells can be found in the ESI (Fig. S3†).
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| Fig. 5 Histograms of flow cytometry analysis of ES2 cells after 24 h (A, C) and 48 h (B, D) of uptake. In (A, B) cells had been incubated with Rh6G-loaded containers, the black curves correspond to high container concentration, the red curve to low container concentration, and the blue curve to a control experiment without containers. Figures (C, D) show the same experiment for TD4-loaded containers. The significant shift in the fluorescence distributions reveals the efficient container uptake. | ||
A summary of the complete flow cytometry analysis is presented in Table 1. To discriminate the cell populations incubated with containers from the control cells without containers, a threshold was set at the 98-percentile of the control sample histogram. The numbers in the table represent the percentage of cells above this threshold for the two cell types, the two container concentrations, and the two incubation times.
| Cell type | MRC5 | ES2 | ||||||
|---|---|---|---|---|---|---|---|---|
| Container load | Rh6G | TD4 | Rh6G | TD4 | ||||
| Concentration | Low | High | Low | High | Low | High | Low | High |
| 24 h uptake | 6% | 15% | 30% | 45% | 6% | 61% | 49% | 77% |
| 48 h uptake | 18% | 38% | 50% | 80% | 32% | 98% | 33% | 77% |
For MRC5 cells, the uptake was significantly higher when incubated with high container concentration, compared to that when incubated with low container concentration (p < 0.01 according to the Kolmogorov–Smirnoff test applied to the selected histograms). Moreover, the uptake increases significantly from 24 to 48 h of incubation (p < 0.01). The same increase with time and container concentration was observed for ES2 cells incubated with Rh6G-loaded containers (p < 0.01).
When ES2 were cultured with TD4-loaded particles, uptake also increased significantly with suspended container concentrations. Instead, an inverse trend was observed regarding the dependence on incubation time. The percentage of cells above uptake-threshold decreased for both container concentrations (p < 0.01), although at high concentration the numbers were comparable (Table 1).
This may be due to the higher ES2 cell metabolism, possibly causing either an earlier release of containers by the cells or the disruption and detachment of TD4 molecules from the particles. This faster metabolic activity of ES2 cells is further confirmed by the generally higher percentage of cells above the uptake-threshold with respect to MRC5 cells under the same culture conditions. The fact that this shows up in TD4-loaded cells only is another indication that dye release from the containers happens much faster for Rh6G- than for TD4-loaded containers, as observed in solution (Fig. 2). This also agrees with the observation from the confocal microscopy that Rh6G immediately stained the mitochondria, while TD4 remained confined within the containers after 24 hours (Fig. 4).
Further studies on the uptake mechanism were performed by additional staining of the lysosomes via the LysoTracker probe (blue channel in Fig. S4†). Lysosomes represent the last stage of the endocytosis pathway and are responsible for the digestion of molecules uptaken by cells. The experiments showed a partial co-localization of Rh6G and TD4 with the lysosomes in the ES2 and MRC5 cells. This indicates an active uptake via endocytosis. To study which endocytotic pathways were involved, uptake efficiencies have to be measured while blocking single pathways.30
Further studies are needed to fully characterise the crystal phase transition and the associated burst release directly within the cells. At the same time, the universality of vaterite containers can be exploited by implementing functional coatings allowing one to actively trigger substance release by external controls such as temperature, ultrasound, or light exposure.
Footnotes |
| † Electronic supplementary information (ESI) available: Images of ES2 and MRC5 cells at different culturing times after adding Rh6G- and TD4-loaded containers; images visualising mitochondria morphology differences between fibroblasts and tumor cells via staining with Rh6G-loaded containers; the FACS data for MRC5 cells. See DOI: 10.1039/c3bm60141b |
| ‡ These authors contributed equally. |
| This journal is © The Royal Society of Chemistry 2013 |