Shashwat S. Banerjeea,
Archana Jalota-Badhwarb,
Prateek Watec,
Sneha Asaia,
Khushbu R. Zopea,
Russel Mascarenhasa,
Dimple Bhatiab and
Jayant Khandare‡*a
aNCE-Polymer Chemistry Group, Piramal Life Science Ltd., Goregaon, Mumbai-400063, India. E-mail: jayant.khandare@mitpune.edu.in
bCancer Biology Group, Piramal Healthcare Ltd., Goregaon, Mumbai-400063, India
cMaterials Science and Engineering, University of Florida, Gainesville, FL 32608, USA
First published on 21st August 2013
Carbon nanostructures such as multiwalled carbon nanotubes (CNT) and graphene (G) are potential candidates in a large number of biomedical applications. However, there is limited understanding and connection between the physicochemical properties of diverse carbon nanostructures and biological systems, particularly with regard to cellular responses. It is also crucial to understand how the structure and surface composition of carbon nanostructures affect the cellular internalization process. Here, through in vitro cellular entry kinetics and cytotoxicity studies using MCF-7 breast cancer cells and H460 human lung cancer cells, we show that the structure and surface composition of CNT and G conjugates with various molecules such as PAMAM dendrimers (G4) and G4-poly(ethylene glycol) (PEG) are directly related to their cellular internalization ability and toxicity. Interestingly, the cellular association of CNT and G nanoconjugates was observed to be structure and surface composition dependent. We found that CNT conjugates internalized more compared to G conjugates. Furthermore, G4 conjugated CNT internalized more compared to G4-PEG conjugated CNT, whereas, higher internalization was found for G4-PEG conjugated G than G4 conjugated G. We have also correlated the cytotoxicity and cellular uptake mechanisms of CNT, G, and their conjugates through zeta potential measurements, fluorescence quenching studies and by fluorescence-activated cell sorting. Altogether these studies suggest different biological activities of the carbon nanostructures, with the shape and surface composition playing a primary role.
CNTs are among the most promising nanoparticles for applications in the biomedical field due to their quasi-one-dimensional (1D) nanostructure, ultra high surface area, unique optical and electronic properties, and better biocompatibility, thus making a “smart” nanoparticle-based system for drug delivery and in vivo bioimaging.5–7 The use of CNTs in the targeted delivery of biomolecules into biological systems carries enormous medical and commercial potential. However, a detailed understanding of their cellular internalization mechanism, intracellular dynamics, and biological toxicity is of paramount importance for the development of these nanomaterials as drug delivery vehicles.
Similarly, G, a two-dimensional (2D) nanomaterial, has attracted tremendous attention due its novel physical properties and potential applications in nanoelectronic devices, transparent conductors, and nanocomposite materials.8–13 Apart from the interest in electrical applications, G based materials are exciting candidates for exploration in biology and medicine, including biodevices, disease diagnosis, and drug delivery systems.2,14,15 A key issue that needs to be understood in the implementation of carbon allotrope nanomaterials such as G and CNTs in a large range of biological applications are their biological responses. Although the two materials have a similar crystalline structure and chemical composition, their interactions with cell systems are expected to be governed by different mechanisms due to their different structures (flat atomic sheets for G and tubular for CNTs). The cellular kinetics, intracellular dynamics, and potential toxicity of G are expected to be significantly different when compared to those of 1D CNTs.16,17 Such studies would provide an insight into the interaction between physically diverse carbon nanostructures and various biological systems both in vitro and in vivo. Furthermore, the new nanomaterials that are being designed and considered for the systemic delivery applications essentially must be evaluated for their structure–activity and biocompatibility relationship even for the possible interactions with plasma proteins.18 Such studies will reflect more light on the biocompatibility profile, and the fate of the nanocarriers in circulation. Recently, we have reported the implications of enhanced cell interactions using 3D surfaces and magneto-dendritic nanoparticles enriched with transferrin as an interacting ligand for accounting cell morphology and capturing circulating tumor cells.19,20 Cellular delivery, tissue distribution and cytotoxicity studies of CNTs and G have directed their use as novel drug delivery nanosystems.1,4 Conjugation of G4 and PEG polymers may enhance the dispersion ability of CNTs and G. However, the enhanced solution properties of these materials may alter the cellular uptake kinetics and may further impart additional cytotoxicity.
In order to fill this knowledge gap, we have systematically investigated the effects of structure and surface composition of physically diverse carbon nanostructures, CNTs and G, on a series of cellular responses including their cellular uptake, internalization mechanisms, intracellular trafficking, and toxicity. To further understand the effect of structure along with surface composition we manipulated CNTs and G by conjugating with G4 and PEG (Fig. 1). To the best of our knowledge, this is the first study to address the cellular uptake and internalization fate for CNTs, G and their conjugates with PAMAM G4 dendrimers and PEG in an identical set of in vitro milieu, combined with a range of cytotoxicity studies. Furthermore, we investigated the difference in cellular internalization of CNTs, G and conjugated nanocomponents by a series of fluorescence-activated cell sorting (FACS) studies. We correlated the cellular internalization of these materials to rationalize the cellular uptake differences with their free forms.
Fig. 1 Schematic illustration of CNT–G4, CNT–G4–PEG, G–G4, and G–G4–PEG nanoparticles. |
Percentage viability was calculated as:
(A × 100)/C |
X-Ray diffraction (XRD) analyses were performed using a Bruker AXS A8 (Germany) X-ray diffractometer with Cu-Kα radiation (1.5405 Å). The Zeta potential was measured using a Beckman coulter (Delsa Nano C, USA) instrument and 0.01 M phosphate buffers at pH 7.4. Solutions of the CNT and G nanosystems were freshly prepared by dissolving an appropriate amount of sample in buffer solution. The sample solutions were then stirred thoroughly to ensure proper mixing of the samples. Zeta potential was measured by applying an electric field across the solutions using the technique of laser Doppler anemometry. Each sample was measured three times, combining 64 runs per measurement. All measurements were carried out at 25 °C.
CNT–G4–Cy5 and CNT–G4–PEG–Cy5 were synthesized from carboxylated CNT (CNT–COOH). Oxidation treatment, an effective approach to eliminate the contaminants and concomitantly generate abundant carboxylic groups at the defect sites of CNTs to result in CNT–COOH, was adopted as the primary step.21 After that, PAMAM G4 dendrimers (64 amine groups per dendrimer molecule) were conjugated through amide linkage by EDC coupling method to yield CNT–G4. Dendrimers are known to form stable, dense, well-organized, and close-packed arrays on the substrate surface, and can significantly improve the dispersibility of CNT and other materials.4 They also provide useful reactive groups for further functionalization. Next, CNT–G4–PEG was synthesized by treating CNT–G4 with the NHS ester of PEG, which is known to make the nanosystem biocompatible and dispersible in aqueous media, at pH 7.8. To impart fluorescence imaging capability, Cy5 was covalently bonded with the excess amine groups of G4 present on CNT–G4–PEG by co-condensation reaction to form the CNT–G4–PEG–Cy5 conjugate. Similarly, Cy5 was conjugated to CNT–G4 to yield CNT–G4–Cy5. At every step, the CNT based reactants were isolated by centrifugation, thereby eliminating unreacted G4, PEG, and Cy5.
On the other hand, G–G4–Cy5 was synthesized by conjugating PAMAM G4 dendrimers to G with surface carboxyl groups via amide formation using the excess terminal amine groups present on PAMAM G4 (Fig. 3). G–G4–PEG was synthesized by conjugating G–G4 with PEG through the NHS ester group to yield the multicomponent system. Further, Cy5 was covalently bonded with excess amine groups of G4 present on G–G4 and G–G4–PEG by co-condensation reaction to form the G–G4–Cy5 and G–G4–PEG–Cy5 conjugates.
CNT and G nanosystems were evaluated to determine their physicochemical properties. The structures of CNT, G and G–G4 (representative figure) were investigated by TEM. Fig. 4A shows the average diameter of CNT to be ∼8 nm, while the TEM image of G (Fig. 4B) shows overlaid side-by-side sheets, varying between 100 and 110 nm in diameter. The TEM image of G–G4–Cy5 (Fig. 4C) did not show any major change compared to G revealing that the conjugation of G4 and Cy5 did not result in agglomeration or degradation of the G. The content of G4 was not analyzed, due to unsuitable method in the literature. Analysis by dynamic light scattering (DLS) showed that the average diameters of CNT, G, CNT–G4–Cy5, G–G4–Cy5, CNT–G4–PEG–Cy5 and G–G4–PEG–Cy5 in water were 146, 296, 296, 336, 327 and 398 nm (Fig. 5A). Because most of the CNT and G-based materials are not spherical particles, the model derived diameters are not their real sizes. DLS results only show size differences among the four materials. It revealed that the size of CNTs and G increased on conjugating with G4, PEG and Cy5. The increase in the size was in the order of G–G4–PEG–Cy5 > G–G4–Cy5 > G > CNT–G4–Cy5 > CNT–G4 > CNT.
Fig. 4 TEM images of oxidized (A) CNTs, (B) graphene and (C) G–G4–Cy5. |
Fig. 5 (A) Hydrodynamic size distribution and (B) zeta potential measurements performed for CNT and G nanosystems. |
Besides the sample's morphologies, their zeta potentials were measured in PBS of pH 7.4 at room temperature. The zeta potential is a measure of electrostatic interactions between colloidal particles and has been used in the literature to investigate the surface charge and the stability of colloidal nanoparticles. Herein, CNTs, G and their conjugates were investigated to account for the effect of conjugation on surface charge. Fig. 5B shows that in both CNTs and G the zeta potential is negative i.e. −1.26 ± 0.09, and −1.48 ± 0.063 mV, respectively. However, on conjugation with G4 and PEG the zeta potential values of the nanomaterials changed to −1.84 ± 0.18, −2.77 ± 0.10, −0.17 ± 0.04 and −0.26 ± 0.04 mV for CNT–G4–Cy5, G–G4–Cy5, CNT–G4–PEG–Cy5 and G–G4–PEG–Cy5, respectively. The results showed that the zeta potential of CNT–G4–PEG–Cy5 is less negative than that of CNTs and CNT–G4–Cy5. Similarly, in the case of G and G conjugates the zeta potential of G–G4–PEG–Cy5 is less negative than that of G and G–G4–Cy5. The change in zeta potential of the CNT and G conjugates compared to CNT and G confirms the conjugation. Passivation molecules such as PEG are neutral.24 Also, the NH2 groups of G4 were utilized during conjugation of PEG. Hence, the PEG conjugated nanosystems showed a lower zeta potential compared to other CNT and G nanosystems.
To study the interactions of CNT and G nanosystems with protein in vitro, BSA was considered as a suitable protein candidate as it is found in abundance in plasma and due to its complimentary structural similarity with human serum albumin.25,26,30 A BSA fluorescence quenching assay system was used to investigate the protein interaction with CNT and G4 and also the effect of G4 and PEG functionalization. BSA exhibits a characteristic emission spectrum of the tryptophan fluorophore. For CNT and G and their conjugates with BSA, changes in the intensity of the emission spectra of BSA upon addition of CNT and G nanosystems were determined. The effect of CNT and G nanosystems on BSA fluorescence intensity is depicted in Fig. 6. When different amounts of CNT and G were added to a fixed concentration of BSA, a significant decrease in the fluorescence intensity of BSA was observed, indicating a strong interaction between BSA and CNT or G. In contrast, the decrease in fluorescence intensity for the CNT and G conjugates suggested a much weaker binding interaction to BSA.
Fig. 6 Stern–Volmer curves of F0/F vs. concentration of CNT and G nanosystems at different temperatures. The concentration of BSA was 2.5 μM. |
As is evident from Fig. S1,† the distinct decrease in the fluorescence intensity upon addition of CNT and G nanosystems can be employed in studying their interaction with BSA. In order to gain a further insight into the binding affinity, fluorescence quenching data were analyzed by the Stern–Volmer equation:20,31–33
F0/F = 1 + kqτ0[Q] = 1 + Ksv[Q] | (1) |
The quenching process was considered to be diffusion controlled with a distinct peak maximum at around 340 nm in buffered aqueous solution. As the quenching process is diffusion controlled and completely dynamic, one can calculate the individual bimolecular quenching constants, kq, by taking the ratio of Ksv and τ0. For BSA, the excited state lifetime of the fluorophore is ∼5 ns.34 The kq values determined for CNT, CNT–G4–Cy5, CNT–G4–PEG–Cy5, G, G–G4–Cy5, and G–G4–PEG–Cy5 were 3.24 × 109, 1.28 × 109, 1.28 × 109, 1.84 × 109, 0.38 × 109 and 0.76 × 109 L g−1 s−1, respectively. The maximum kq value of BSA for diffusion-limited quenching (dynamic mechanism) possible in water is ∼1.5−5 M−1 L g−1 s−1.35 The kq values determined were larger than the limiting diffusion rate constant of the albumin molecule. A higher kq value reveals that static quenching may be present in the system. However, it is difficult to state whether the fluorescence quenching of the tryptophan fluorophore by the nanosystems is predominantly static or dynamic in nature. Earlier, we reported the influence of surface functionalities and zeta potential by fluorescence quenching studies to address the binding interactions of dendritic polyglycerols (dPG) and other delivery polymers with BSA in order to explore the applicability of dPG derivatives for systemic delivery.20 In general, the interaction of nanocarriers with plasma proteins are highly associated as either +ve type or −ve type and with the total surface charge. Furthermore, the high protein interactions are associated with the change in the physical nature and conformation of the protein and may result in extended pharmacokinetics of these nanomaterials.20 The correlation of such protein interactions either as dynamic or static (or mixed), may be implicated in reversible or irreversible plasma protein binding.
As revealed from the fluorescence measurements, the effect of CNT and G nanosystems on the quenching of tryptophan was clearly ranked in the order CNT–G4–PEG–Cy5 > G–G4–Cy5 > G–G4–PEG–Cy5. Our spectroscopic results, therefore, imply that the interaction of the negatively charged BSA with CNT and G nanosystems is mainly due to electrostatic interactions.
The cellular internalization kinetics of CNTs, G and their conjugates were followed for 2–24 h. The cellular association of CNT and G conjugates were found to be time dependent, with red fluorescence due to Cy5 being detectable in the cells as soon as after 2 h of incubation at 37 °C (Fig. 7). During the first 6 h, these particles were observed in the cytoplasm (Fig. 8). However, at 24 h (Fig. 9), a higher amount of CNT and G nanosystems were observed in the cells compared to 6 h. The cellular internalization of the nanosystems was also confirmed by Z-stack imaging (Fig. S2 of CNT–G4–PEG–Cy5 in ESI†) of MCF-7 cells. To further understand the cell internalization kinetics of the CNT and G conjugates, the extent of cellular uptake of the various conjugates was quantified by determining the fluorescence of Cy5 from the treated MCF-7 and H460 cells using flow cytometry. The cellular internalization kinetics were followed for 4, 8, 16, 24 and 48 h (Fig. 10 and S3†). Both CNT and G conjugates were internalized in the cells within 4 h of treatment, which correlates well with the CLSM study. All the cells were found to be stained within 4 h of treatment. The median fluorescence intensity (MFI) for these nanoparticles was in the order CNT–G4–Cy5 > CNT–G4–PEG–Cy5 > G–G4–Cy5 > G–G4–PEG–Cy5 for all the time points (Fig. 10D). This observation shows that the CNT conjugates were internalized more than the G conjugates. This can be explained on the basis of the physical properties of CNT and G conjugate nanosystems. While the cellular uptake is influenced by the size, more recent studies have also demonstrated the significant impact of shape on the cell dynamics.36–38 The rate and the intracellular fate of the nanosystems uptake by cells depends on factors such as charge and structure. CNT, due to the “snaking” effects, because of their tubular shape, promotes penetration of membranes, uptake by cells, and strong interactions with various protein systems.8 Hence, a higher uptake of CNT conjugates compared to G conjugates are observed over time. This is an important observation and underlines the implications of the shape of nanoparticles in modulating biological phenotype.
Fig. 7 Confocal laser scanning microscopic images of MCF-7 cells incubated with CNT–G4, CNT–G4–PEG, G–G4, and G–G4–PEG nanoparticles for 2 h. (A) Left: merged images of the nuclei stained with blue DAPI and Cy5 conjugated CNT–G4, CNT–G4–PEG, G–G4, and G–G4–PEG nanoparticles. Middle: merged images of the nuclei stained with blue DAPI, Cy5 conjugated CNT–G4, CNT–G4–PEG, G–G4, and G–G4–PEG nanoparticles and differential interference contrast (DIC). Right: differential interference contrast (DIC) images. |
Fig. 8 Confocal laser scanning microscopic images of MCF-7 cells incubated with CNT–G4, CNT–G4–PEG, G–G4, and G–G4–PEG nanoparticles for 6 h. (A) Left: merged images of the nuclei stained with blue DAPI and Cy5 conjugated CNT–G4, CNT–G4–PEG, G–G4, and G–G4–PEG nanoparticles. Middle: merged images of the nuclei stained with blue DAPI, Cy5 conjugated CNT–G4, CNT–G4–PEG, G–G4, and G–G4–PEG nanoparticles and differential interference contrast (DIC). Right: differential interference contrast (DIC) images. |
Fig. 9 Confocal laser scanning microscopic images of MCF-7 cells incubated with CNT–G4, CNT–G4–PEG, G–G4, and G–G4–PEG nanoparticles for 24 h. (A) Left: merged images of the nuclei stained with blue DAPI and Cy5 conjugated CNT–G4, CNT–G4–PEG, G–G4, and G–G4–PEG nanoparticles. Middle: merged images of the nuclei stained with blue DAPI, Cy5 conjugated CNT–G4, CNT–G4–PEG, G–G4, and G–G4–PEG nanoparticles and differential interference contrast (DIC). Right: differential interference contrast (DIC) images. |
Furthermore, the results also revealed that CNT–G4–PEG–Cy5 internalized less compared to the CNT–G4–Cy5 conjugate, as seen in Fig. 10. This observation can be explained on the basis of the electrostatic force between the nanosystem and the cell surface. Since CNT–G4–PEG–Cy5 has a higher negative surface charge (Fig. 5), it encounters strong electrostatic repulsions with the cell wall. Hence, less internalization of CNT–G4–PEG–Cy5 was observed compared to CNT–G4–Cy5. On the other hand, G–G4–PEG–Cy5 was internalized more because it has less negative charge than G–G4–Cy5. This observation reinforces that, along with structure, the charge of the conjugate is crucial for cell uptake.
The cellular internalization for the CNT and G nanoconjugates was found to be at a maximum at 24 h as evident from Fig. 10 and S3.† The number of positively labeled cells were represented as the percentage of total cell counts in Fig. 10. More than 90% of the cells were positively labeled at 24 h for CNT and G conjugates except for G–G4–Cy5 (Fig. S4†). Similar results were also seen for H460 cells (Fig. S5†).
Fig. 11 Results of the PI (propidium iodide) cytotoxicity assay on MCF-7 breast cancer cells after an incubation period of 72 h with various samples of CNT at concentrations ranging from 0–10 μg mL−1; *P < 0.05. |
Interestingly, the CNT and G conjugates exhibited less cytotoxicity pattern than that exhibited by CNT and G. These toxicity findings can be elucidated by the structure of these nanomaterials and their biological interaction with the cellular systems. As previously discussed, CNTs promote the rapid penetration of membranes, uptake by cells, and strong interactions with various protein systems due to the “snaking” effects.8 The G nanostructures, due to their flat shapes, have stronger interaction with the cellular membrane thus enabling higher cell internalization.38 However, by conjugating other nanocomponents to CNT and G, the cellular internalization differed. Although CNT and G conjugates have a core with same chemical formula i.e. CNT and G, they differ only in hydrodynamic size and Z-potential values. Hence, the difference in the cell entrance pattern can be mainly attributed to structure and surface composition of the functionalized CNT and G. Similar results were also seen for H460 cells (Fig. S6†).
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c3bm60082c |
‡ Present address: Maharashtra Institute of Pharmacy MIT Campus, Paud Road, Kothrud, Pune-411038, India. |
This journal is © The Royal Society of Chemistry 2014 |