Mengli Dinga,
Borja Moreira-Álvarez*b,
Francisco Calderón Celis*b,
Jose Manuel Costa-Fernándezb,
Jorge Ruiz Encinarb and
Ruxandra Gref*a
aInstitut des Sciences Moléculaires d’Orsay, Centre National de la Recherche Scientifique (CNRS), Université Paris-Saclay, 91405 Orsay, France. E-mail: ruxandra.gref@universite-paris-saclay.fr
bDepartment of Physical and Analytical Chemistry, University of Oviedo, Avenida Julian Claveria 8, 33006, Oviedo, Spain. E-mail: borjamoreira@gmail.com; calderonfrancisco@uniovi.es
First published on 5th January 2024
Nanosized UiO66 are among the most studied MOF materials. They have been extensively applied in various areas, such as catalysis, gas absorption, electrochemistry, chemical sensing, and biomedical applications. However, the preparation of stable nano-sized UiO66 for drug delivery applications is challenging because of the high tendency of UiO66 to aggregate during storage. To address this issue, we coated UiO66 with oligomers made of crosslinked cyclodextrins. The coated UiO66 exhibited a good stability upon storage for more than three weeks, even for low quantities of coating materials. The resulting core–shell UiO66 were characterized using a set of complementary methods including microscopies, spectroscopies, X-ray diffraction, and thermogravimetric investigations. Size distribution was assessed by orthogonal methods. Cisplatin was loaded in the core–shell nanoparticles, followed by an in-depth analysis by asymmetric flow field-flow fractionation (AF4) hyphenated with inductively coupled plasma-mass spectrometry (ICP-MS). This method combines the extremely high elemental selectivity and ultratrace detection limits of mass spectrometry with the capacity of AF4 to differentiate the diverse populations present in the sample. Free cisplatin and UiO66-associated cisplatin could be well separated by AF4. AF4-ICP-MS/MS analysis provided the exact drug loading, without the need of separating the nanoparticles from their suspension media. These data suggest the potential of AF4-ICP-MS/MS in the optimization of drug delivery systems.
In particular, UiO66 draws increasing attention, especially since the reported synthesis of defected UiO66.7,8 In 2017, Morris et al. added modulators (acetic, formic, dichloroacetic, or trifluoroacetic acids) during UiO66 preparation in an attempt to improve their physicochemical properties.7 The modulators competed with the organic ligands in coordinating with the metal ions, resulting in the formation of defects in the crystalline structure, which in turn enhanced UiO66's colloidal stability. By controlling both the chemical structure of the modulators and their concentrations, it was possible to modulate the size of the UiO66 within a large range, from less than 50 nm to more than one micron. However, the long term storage stability of UiO66 still needs to be improved.
To circumvent this stability problem, attempts were made to engineer core–shell nanoplatforms by coating UiO66 with chitosan, polydopamine, silica, and other polymers.9–12 For instance, Trushina et al. coated UiO66 with SiO2 resulting in improved colloidal stability in various physiological media.12 However, both the porosity and drug loading ability of UiO66 decreased after coating with SiO2. In other approches, UiO66 were coated with poly(ethylene glycol) (PEG) by click chemistry without affecting their porosity.13 Nevertheless, the synthesis was complex and required the use of large amounts of organic solvents. Therefore, there is a clear need to develop stable core–shell UiO66 nanoMOFs using a simple and green strategy that has no effect on the nanoparticles' porosity.
Due to their well-known biocompatibility and versatility, cyclodextrin (CD) derivatives such as phosphate-CDs (CD-P), polymerized CDs, and CD-based oligomers have been investigated as coating materials to improve nanoMOFs' stability.14–16 Since 2015, our group has been working on the improvement of nanoMOFs stability without affecting their porosity and drug loading ability.14 Functionalized CDs spontaneously anchored onto the surface of MIL100 nanoMOFs. Further coating optimizations were made through the cross-linking of CDs with citric acid first,15 and malic acid later on.16 The resulting CD oligomers could advantageously be functionalized with PEG, and fluorescent molecules. The coated nanoMOFs exhibited good storage stability, and the presence of the coating did not affect porosity and drug loading capacity. However, to our knowledge, the CD-based coatings were only studied on MIL100 and not on other nanoMOFs such as UiO66.
In the last decades, UiO66 nanoMOFs have been widely used as carriers to treat pulmonary diseases, infections, and cancer.17–20 The size of the drug molecules should be smaller than UiO66's windows to enable drug diffusion into the porosity, ensuring an efficient loading. One example of an appropriate drug for loading in UiO66 is cisplatin, the most extensively applied anticancer drug for the treatment of several cancers.21–23 Cisplatin and its prodrug have been successfully loaded within the porosity of UiO66, functionalized or not with amine moieties.18 The presence of cisplatin in the UiO66 was assessed by energy-dispersive X-ray spectroscopy and microwave plasma-atomic emission spectroscopy. Cisplatin loadings reached 4.7 wt%, and 48% of the drug was released within 24 h. However, the spectroscopic techniques used to assess drug loading have poor energy resolution and low sensitivity. In fact, an accurate assessment of cisplatin's loading into UiO66 nanoMOFs would require a very selective and sensitive analytical method.
In this sense, asymmetric flow field-flow fractionation (AF4), in conjunction with more traditional spectroscopic techniques (e.g., UV-Vis, MALS, etc.) has established itself as a powerful analytical tool to characterize nanomaterials,24 and even to assess their drug delivery properties.25,26 Particularly, hyphenated with inductively coupled plasma-mass spectrometry (ICP-MS), AF4-ICP-MS combines the extremely high elemental selectivity and ultratrace detection limits of the mass spectrometry with the capacity of AF4 to differentiate the diverse nanoparticle populations present in the sample.27,28 However, to the best of our knowledge, it has not been applied so far to study drug loading in nanoMOFs.
We aimed here to gain a deep understanding on cisplatin loading into UiO66 nanoMOFs using AF4-ICP-MS/MS. Another novelty here was to coat UiO66 nanoMOFs with CD oligomers by a simple, and organic solvent-free method, to obtain stable, uniform nanoparticles with low toxicity. The coating materials had no effect on UiO66's porosity. Bare and coated UiO66 nanoMOFs were characterized by complementary techniques, such as Transmission Electron Microscopy (TEM), Dynamic Light Scattering (DLS), Nanoparticle Tracking Analysis (NTA), and Tunable Resistive Pulse Sensing (TRPS), to determine their size distribution and morphology. The nanoMOFs' porosity, crystallinity, stability, composition, and toxicity on macrophage J744 cells were investigated. The exact cisplatin incorporation yield and drug distribution within CD-MO@UiO66 were clearly evidenced by AF4-ICP-MS/MS. Noteworthy, the methodology used here avoids the need of separating the nanoMOFs from their suspension media which can lead to artefacts. In a nutshell, we show the ability of AF4-ICP-MS/MS to characterize the cisplatin loaded nanoMOFs throughout the encapsulation process. These investigations set the basis for using AF4-ICP-MS/MS as a diagnostic tool in drug loading and delivery studies.
The mean hydrodynamic diameter and polydispersity (PDI) of nanoMOFs were analyzed by DLS (Malvern Panalytical, Nano-ZS, Zetasizer Nano series, Palaiseau, France). Samples were diluted with water at the final concentration of 50 μg mL−1, and the experiment was carried out at 25 °C and an angle of 90°. Experiments were performed in triplicate. Colloidal stability of the uncoated and CD-MO-coated UiO66 was also studied by DLS. To do so, UiO66 and CD-MO@UiO66 nanoMOFs were stored at 4 °C, and analyzed up to 21 days.
The Zeta potential (ZP) of UiO66 and CD-MO@UiO66 in a pH range of 3–9 was determined using a Zetasizer instrument (Malvern Panalytical Nano-ZS, Zetasizer Nano series, Palaiseau, France).
Nanosight (LM10, Malvern Instruments Ltd, Palaiseau, France) was employed to determine both the size distribution and concentrations of nanoMOFs by NTA. The method combines a conventional optical microscope with a laser to illuminate the nanoMOFs in their Brownian motion, and the trajectories are determined using a camera. This enabled to further calculate both the size distribution and the nanoparticle concentration. Results are expressed as the mean of five independent measurements.
TRPS (qNano Gold, Izon, Christchurch, New Zealand) was used to analyze the size distribution of the nanoparticles as they passed through a size-tunable NP200 nanopore. To do so, 1x DPBS was filtered twice with 0.22 μm filters before use as electrolyte. The system was calibrated using 200 nm polystyrene standards at a concentration of 8.2 × 1011 particles per mL and the standard was diluted 1000 times before usage. The stretch of the nanopore (48.85 mm), the voltage (0.46 V), the current (120 nA), pressure (19.82), and particle rate (650 particles per min) were fixed for all the experiments. The freshly prepared nanoparticles were diluted with 1x DPBS to obtain a final concentration of 25 μg mL−1.
The porosity of the UiO66 nanoMOFs before and after coating was determined using an ASAP 2020 (Micromeritics, USA). To measure the Brunauer–Emmett–Teller (BET) surface areas of UiO66 before and after coating with CD-MO oligomers, the samples were first dried at 60 °C overnight to remove free water. After additional degassing at 100 °C overnight, samples were analyzed at −196 °C under high vacuum.
The crystallinity of uncoated and CD-MO-coated UiO66 was investigated by powder X-ray diffraction (PXRD). The experiments were carried out on the MORPHEUS platform at the Laboratoire de Physique des Solides (Université Paris-Saclay, Orsay, France), with a home-made diffraction setup installed on a rotating anode generator (model RUH3R, Rigaku Corp., Japan) at the Cu wavelength (λCuKα = 0.1542 nm) delivered by a multilayer W/Si mirror (Osmic). NanoMOFs powders were filled in cylindric borosilicate capillaries (diameter of 1 mm, WJM-Glass Müller GmbH, Berlin, Germany). Diffraction patterns were collected on a large-area detector MAR345 (marXperts GmBH, Germany) with 150 μm pixel size. The experimental resolution is a Gaussian function with full-width at half-maximum equal to 0.013 Å−1. Extraction of the scattered intensity I as a function of the scattering angle 2θ was obtained from the azimuthal angular integration [0, 2π] of the diffraction patterns with a home-made developed software.
Thermogravimetric analyses (TGA, TGA 4000 Instruments, PerkinElmer, 100–240 V/50–60 Hz) were performed to analyze the composition of UiO66 and to determine the associated amounts of CD-MO oligomers. Samples were first dried at 60 °C in an oven overnight. Approximately 20 mg of samples were accurately weighted and heated from 30 to 600 °C at a heating rate of 3 °C min−1 with an oxygen flow of 20 mL min−1. The association efficiency of CD-MO on UiO66 was calculated based on the dried weight and the mass of residues in CD-MO@UiO66. In addition, the composition of the UiO66, CD-MO oligomers, and CD-MO@UiO66 as dried powders was analyzed by Attenuated Total Reflectance (ATR, PerkinElmer, FT-IR Spectrometer, UATR Two).
The hydrodynamic diameters and PDI of UiO66 were further analyzed with DLS. As most applications of nanomedicine involve solutions, the hydrodynamic diameter is crucial to correlate nanoparticle sizes with physiological responses.31 As illustrated in Fig. 2A, the mean hydrodynamic diameters of UiO66 were around 130 ± 3 nm, consistent with TEM observations (Fig. S1A†). The low PDI value (0.037 ± 0.024) indicated the narrow UiO66 nanoMOFs size distribution in agreement with TEM investigations. Fig. S2† showed the DLS size and intensity distributions. Despite its universality and simplicity, DLS only allows to study whole populations of NPs. On the opposite, NTA enables to determine the hydrodynamic diameters of individual NPs, as well as the concentration of the NP suspensions, offering in deep quality control of the formulations.32 As shown in Fig. 2A (black line), the average NTA size of UiO66 nanoMOFs was 109 ± 5 nm, in agreement with TEM evaluations.
Fig. 2 Average hydrodynamic diameters of (A) UiO66 nanoMOFs and (B) CD-MO@UiO66 obtained by DLS (number distribution), NTA and TRPS. |
In TRPS, the mean diameter of individual NPs is measured individually as they pass through a size-tunable nanopore. NP size is directly proportional to pore blockade magnitude.33–35 The TRPS size of UiO66 was 105 ± 30 nm (Fig. 2A, blue line). Noteworthy, Fig. 2A shows the good agreement between the different techniques used to determine the size distribution of UiO66 nanoMOFs, highlighting their homogeneous size distribution.32,33,36
Investigated by TEM, CD-MO@UiO66 showed similar morphologies and sizes (115 ± 22 nm) as naked UiO66 (103 ± 10 nm) (Fig. S1B†). The hydrodynamic diameter of CD-MO@UiO66 was evaluated as 142 ± 6 nm by DLS, similar to the uncoated UiO66. The mean diameters of CD-MO@UiO66 analyzed by NTA and TRPS were 123 ± 41 nm and 115 ± 25 nm, respectively. Fig. 2B presents a comparison of the size distribution of CD-MO@UiO66 obtained by DLS, NTA and TRPS. There is a good agreement among the data obtained by the three independent methods. Comparison of both coated and uncoated UiO66 suggests that the CD-MO coating did not significantly influence the size of UiO66 nanoMOFs. Moreover, NTA allowed determining the concentration of the nanoMOF suspensions, expressed as particle number per mL. This concentration was similar before and after coating (6.2 × 108 ± 2.0 × 107 and 5.7 × 108 ± 1.41 × 107 particles per mL, respectively). These data suggest that there was no aggregation after the coating process.
The associated amounts of CD-MO oligomers on UiO66 were determined by TGA. As shown in Fig. 3A, there were three weight loss steps within the range of 30–600 °C. The first weight loss step from 30–200 °C corresponds to the evaporation of free and associated water within the UiO66 pores. Then, in the second weight loss step, CD-MO oligomers started to degrade from about 200 °C until complete mass loss at around 600 °C. The amount of associated CD-MO was determined based on the amounts of dried samples and their residues. The association amounts of CD-MO oligomers on UiO66 was 5 wt%.
The crystalline structure of uncoated and CD-MO-coated UiO66 was investigated by PXRD. Fig. 3B shows similar PXRD patterns of UiO66 and CD-MO@UiO66, suggesting that the CD-MO coating did not affect UiO66's crystalline structure. Similar results were also found in the infrared spectra of bare and coated UiO66 nanoMOFs (Fig. 3C). There were no obvious differences between UiO66 and CD-MO@UiO66, indicating that the CD-MO coatings did not affect the chemical composition of the UiO66.
High nanoMOFs porosity and BET surface areas are critical for drug delivery applications. Here, the porosity of UiO66 coated or not with CD-MO oligomers was investigated by N2 adsorption experiments (Fig. 3D). As calculated, the BET surface area of UiO66 before and after coating with oligomers was 1494 ± 30 m2 g−1 and 1370 ± 42 m2 g−1 respectively, without significant variation (<10%) between them. This suggested that CD-MO coating did not affect the porosity of UiO66.
ZP measurements enabled to investigate the surface charge of UiO66 coated or not with CD-MO oligomers, in a pH range of 3–9. As shown in Fig. 3E, the ZP of UiO66 showed a pH-dependent profile. When the pH increased from 3 to 9, UiO66's ZP decreased from +35 mV to −30 mV. In contrast, the ZP of CD-MO coated UiO66 was always negative whatever the pH. These dramatic ZP differences supported the successful coating of UiO66 with CD-MO. The colloidal stability of uncoated and CD-MO-coated UiO66 was evaluated in aqueous media (pH 6.5) within three weeks. As illustrated in Fig. 3F, UiO66 aggregated rapidly, and their size became larger than 400 nm within one week. In contrast, the size of CD-MO@UiO66 didn't change for up to three weeks, indicating the good colloidal stability of CD-MO@UiO66. This suggested that the oligomer coating could efficiently improve UiO66's colloidal stability.
Therefore, compared with other types of coatings based on silica or dopamine, the coating with CD-MO offers the advantage of simplicity and avoids the need of organic solvents or reactants,9–12 More importantly, CD-MO coatings did not affect the physico chemical properties of the nanoMOFs.
As shown in Fig. 4, the cell viability was higher than 85% whatever the UiO66 and CD-MO@UiO66 concentrations within the range 0–200 μg mL−1. No IC50 was obtained in this range, achieved within this concentration, suggesting the low toxicity of both naked and coated UiO66 and with further studies, their potential for biomedical applications.
Fig. 5 ICP-MS/MS characterization steps during the preparation process of CD-MO@UiO66-cisplatin. Mass balances refer to the mass of Pt and Zr in A. |
Firstly, the total amount of Zr and Pt within CD-MO@UiO66-cisplatin was determined. ICP-MS/MS analysis of CD-MO@UiO66-cisplatin (Fig. 5A) resulted in a concentration value of 1.04 ± 0.09 mM of Zr and 3.54 ± 0.13 μM of Pt. These results provided a theoretical ratio of 0.020 cisplatin molecules per nanoMOF cell unit, considering that each nanoMOF cell unit contains 6 atoms of Zr (Table 1A). To explore the amount of the cisplatin actually associated with nanoMOFs and therefore to discriminate the free from the associated cisplatin, CD-MO@UiO66-cisplatin MOFs were purified by centrifugation. Metal contents of Zr and Pt in CD-MO@UiO66-cisplatin obtained herein will be regarded as reference (100%) to which compare subsequent quantifications.
Step (Fig. 5) | Sample | Cisplatin/nanoMOF cell unit (Zr6) | Encapsulation efficiency (EE, %) |
---|---|---|---|
A | CD-MO@UiO66-cisplatin | 2.0 × 10−2 | — |
C | Pellet 1 | 6.6 × 10−3 | 27 ± 3% |
E | Pellet 2 | 5.8 × 10−3 | 24 ± 5% |
After a first centrifugation, both Zr and Pt were quantified in supernatant 1 (Fig. 5B) and pellet 1 (Fig. 5C), respectively. ICP-MS/MS quantification revealed that 94 ± 8% of Zr was recovered in the pellet 1, and barely 0.9 ± 0.1% of the Zr in the CD-MO@UiO66-cisplatin nanoMOFs remained in the supernatant. This implies that the nanoMOFs can be efficiently recovered by centrifugation with negligible losses in the supernatant. Nevertheless, the amount of Pt that remains with the nanoMOFs in the pellet 1 is just 27 ± 3%, whereas most of the Pt (64 ± 7%), corresponding to free cisplatin, is found in the supernatant 1. In this way, the molar ratio of Pt/Zr shows a more accurate estimation of the cisplatin drug loading capacity within nanoMOFs, with 0.0066 cisplatins per nanoMOF cell unit (only one out of 151 nanoMOFs cells are occupied with Pt) (Table 1C).
Noteworthy, this value is significantly lower than the theoretical one obtained prior to centrifugation (Table 1A), because of the removal during the centrifugation of all free cisplatin and possibly some loosely adsorbed over the nanoMOFs surface.
However, it cannot be overruled that the centrifugation process may be releasing some of the loaded cisplatin. In order to check this issue, the pellet 1 was redispersed and centrifuged again using the same conditions, and the supernatant 2 (Fig. 5D) and pellet 2 (Fig. 5E) were analyzed. After the second centrifugation, most of the Zr (91 ± 8%) was recovered in the pellet 2, which is consistent with the first centrifugation result.
On the other hand, only 4 ± 1% of the Pt in the supernatant 2 was determined, which hardly corresponded to 15 ± 3% of the Pt present in pellet 1. This means that centrifugation does not seem to release loaded cisplatin. Finally, only 24 ± 5% of the Pt originally added (Fig. 5A) was associated to the nanoMOFs after purification. As most of the Pt is kept in the pellet 2 after the second centrifugation, this Pt can be confidently assumed to correspond to nanoMOF-loaded or tightly associated cisplatin.
As a result, the molar ratio of Pt/Zr determined in the pellet 2 (0.0058 cisplatins per nanoMOF cell unit) (Table 1E), slightly lower than in the pellet 1 due to further purification of free and/or adsorbed cisplatin, shall be a more accurate estimation of the cisplatin loaded into the nanoMOFs. This result highlights the necessity of purification after drug loading process.
The optimum AF4-MALS-ICP-MS/MS instrumental conditions are shown in Tables S1 and S2.† CD-MO@UiO66 nanoMOFs and pure cisplatin were separately injected and analyzed, and the fractograms are shown in Fig. 6. AF4-ICP-MS/MS analysis of CD-MO@UiO66 resulted in a single Zr peak at around 5 min. In the case of pure cisplatin, Pt fractogram showed a single peak at a retention time of 6–7 min, clearly separated from the nanoMOFs peak. This means that the free cisplatin and the nanoMOFs present in the same sample can be well separated using AF4, which enables us to characterize better the species distribution and cisplatin loading efficiency.
Fig. 6 AF4-ICP-MS/MS fractogram of Zr (black, represents for UiO66) in CD-MO@UiO66 sample and Pt (red, represents for cisplatin) in pure cisplatin. |
After the first centrifugation, the Zr signal in AF4-ICP-MS/MS fractograms obtained for both supernatant 1 (Fig. 5B) and pellet 1 (Fig. 5C) were very similar to the ones obtained for the CD-MO@UiO66. This indicates that the only Zr species eluting is the UiO66 nanoMOFs (Fig. 7B and C). In contrast, the Pt peak profiles obtained for the CD-MO@UiO66-cisplatin, pellet 1 and supernatant 1 clearly differ. Unlike the CD-MO@UiO66-cisplatin profile, in which Pt mainly coeluted with Zr, most of Pt was observed to correspond to free cisplatin (Fig. 7B) in the supernatant 1.
Interestingly, as shown in Fig. 7C, there are two peaks observed in the Pt fractograms of redispersed pellet (Fig. 5C), confirming the coexistence of still some free cisplatin and associated cisplatin after the first centrifugation.
Supernatant 2 (Fig. 5D), obtained after the centrifugation of the resuspended pellet 1, hardly contains either nanoMOFs or cisplatin as demonstrated by the very low Zr and Pt total content determined (3 and 4%, respectively). Its AF4-ICP-MS/MS analysis resulted in a similar Pt peak profile as the supernatant 1, with a very dominant peak of free cisplatin eluting at 6 min (Fig. 7D) as it was previously observed for supernatant 1 (Fig. 5B). Most of the Pt and Zr originally present in pellet 1 was found in the new redispersed pellet 2 instead (Fig. 7E). Unlike in the pellet 1 (Fig. 7C), where the Pt signal at the retention time of the free cisplatin was still significant, the vast majority of the Pt signal of redispersed pellet 2 closely followed the Zr (nanoMOFs) profile.
It appears that while the first centrifugation removed most of the un-associated cisplatin (64% of the Pt originally added), the second centrifugation only removed a small portion (4%) of the Pt present after the first centrifugation (27%) that likely corresponded to loosely adsorbed cisplatin onto the surface of nanoMOFs. In fact, it seems that centrifugation does not promote any significant cisplatin release from the nanoMOFs. Therefore, total metal content by FIA-ICP-MS/MS and AF4-ICP-MS/MS results evidence that two centrifugation processes were required to remove completely the un-associated and loosely adsorbed cisplatin. Therefore, the molar ratio cisplatin/nanoMOFs determined for the pellet 2 after the second centrifugation could be considered as an accurate indicator of the actual cisplatin internally (and stably) loaded within the nanoMOFs (Table 1).
FIA-ICP-MS/MS (total element content) in conjunction with AF4-ICP-MS/MS (elemental speciation) proved to be a powerful tool to determine the real drug loading directly on nanoMOFs suspensions, without the need of separation. Indeed, non-encapsulated free cisplatin and loaded cisplatin could be distinguished within the AF4 separation process. The analysis of various samples at different stages of the encapsulation and purification processes gave a clear picture of the incorporation yields and drug distribution within the nanoMOFs and their suspension medium. AF4-ICP-MS/MS appeared to be a sensitive and elegant strategy to provide a strong control over the different production steps, leading to fully characterized drug-loaded MOFs. It could be an asset in the design of other nanomedicines.
This study sets up the basis of a highly sensitive methodology that could be applied to other types of multifunctional nanoparticles, loaded with drugs and with different types of coatings.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ra07098k |
This journal is © The Royal Society of Chemistry 2024 |