Alia
Alkaabi
ab,
Khansa
Ahsan
a,
Nayla
Munawar
a,
Abdelouahid
Samadi
a,
Hesham
El-Maghraby
a,
Amr
Amin
c and
Yaser
Greish
*a
aDepartment of Chemistry, Al Ain, United Arab Emirates. E-mail: y.afifi@uaeu.ac.ae
bDepartment of Biology, United Arab Emirates University, Al Ain, United Arab Emirates
cDepartment of Basic Medical Sciences, College of Medicine, Sharjah University, Sharjah, United Arab Emirates
First published on 5th July 2024
Applications of metal–organic framework (MOF) nanostructures in biomedicine have rapidly expanded over the past decade. MOFs are characterized by their high functionality, surface area, and porosity, providing an ideal platform for several biomedical applications. This study explores the potential of a novel therapeutic approach for liver cancer, incorporating Safranal, a bioactive molecule derived from saffron, within the iron-based metal–organic framework (MOF), MIL-88B(Fe). The successfully loaded Safranal-MIL-88B(Fe) composite nanostructure was comprehensively characterized and tested for its effectiveness against HepG2 liver cancer cells. Furthermore, we investigated its antibacterial efficacy against Escherichia coli (E. coli) and Lactobacillus strains. The proposed mechanism of action of the Safranal-MIL-88B(Fe) nanostructures potentially shows the effect of the release of the ferric ions and Safranal in vitro against HepG2 cancer cells and both bacterial strains. Our findings show significant promise for Safranal-loaded MIL-88B(Fe) as a dual-purpose therapeutic agent, opening exciting avenues for future biomedical applications.
MOFs are porous crystalline materials with coordinating organic ligands and inorganic metal ions (or clusters).4,5 Their intrinsic features, including well-ordered and controllable porosity, remarkable crystallinity, and large surface areas, make them suitable host matrices for immobilizing biomolecules. The Materials of Institute Lavoisier (MIL) series exemplifies these MOF nanostructures, renowned for their remarkable framework flexibility. The unit cells of a number of these MIL nanostructures, such as MIL-88A and MIL-88B, can reversibly swell and shrink without compromising the overall framework topology, a phenomenon known as breathing behavior.6,7 This unique property allows the carrier to adapt its pore size intelligently to accommodate various drugs, subsequently stabilizing sensitive molecules.8
Iron-containing MOFs (Fe-MOFs) have attracted much interest due to their superior safety and biodegradability profiles.9–11 Most Fe-MOFs are members of well-known MIL and BioMOF families, including MIL-53, MIL-88A, MIL-88B, MIL-100, MIL-101, MIL-127, BioMOF-1, and BioMOF-5.12–20 These MOFs have shown great potential as drug carriers, successfully encapsulating and delivering various therapeutic drugs, including busulfan, azidothymidine triphosphate, cidofovir, and doxorubicin.21
Addressing concerns regarding the potential toxicity of metals employed in MOFs, a study has explored a series of fourteen MOFs with varying compositions (Fe, Zn, and Zr; carboxylates or imidazolates). This investigation revealed iron (Fe) as the least toxic metal among those tested.22 Consequently, developing Fe-MOFs with iron as the core metal ion has garnered significant interest due to their unique properties and potential applications. The incorporation of iron introduces a range of additional functionalities, including redox activity, intrinsic peroxidase-like activity, diverse catalytic properties, and even antimicrobial and antifungal properties.23–26
Fe-MOFs also hold significant promise for cancer treatment by inducing ferroptosis in cancer cells, a regulated cell death characterized by iron-dependent lipid peroxidation. These MOFs can trigger ferroptosis through various mechanisms. Firstly, the iron within Fe-MOFs facilitates the Fenton effect, generating highly reactive hydroxyl radicals (˙OH) from hydrogen peroxide (H2O2), leading to oxidative stress and cell death.27 Additionally, Fe-MOFs contribute to producing reactive oxygen species (ROS) within the cancer cells, further disrupting cellular homeostasis and promoting cell death.28–30 Moreover, the iron centers in Fe-MOFs can form coordination bonds with specific anticancer drugs, enhancing targeted drug delivery and controlled release and ultimately improving chemotherapy efficacy.27 These diverse mechanisms highlight Fe-MOFs’ potential as a powerful tool in cancer therapy.
A study on MIL-88B-type multivariate (MTV-1) nanocarriers serves as an example. These nanocarriers, made of a mixed linker and metals (iron and cobalt), contained 5-fluorouracil (5-FU) and curcumin (CUR). MTV-1@5-FU + CUR demonstrated pH-responsive drug release, with more drugs released at pH 5.5 (cancer microenvironment). MTV-1 MOFs also showed peroxidase-like activity and catalyzed H2O2 breakdown in chemodynamic treatment. Cell assays revealed a substantial inhibitory impact against HepG2 cells (IC50 = 78.7 μg mL−1). This demonstrates Fe-MOFs’ potential in combination therapy, as dual-drug loading, pH-responsive release, and chemodynamic therapy hold promise for multifunctional anticancer treatment.31
Safranal, derived from saffron, has been of interest due to its potential pharmacological effects on liver cancer. Safranal demonstrated promising outcomes in decreasing HepG2 cell viability, with an IC50 of 500 μM after 48 hours, highlighting its potential as a liver cancer therapy. Additionally, Safranal induced morphological changes in HepG2 cells, such as rounded shapes, shrinkage, and increased detachment, supporting its cytotoxic effects. Also, Safranal suppressed colony formation in HepG2 cells in a dose-dependent manner, with the most effective concentration at 100 μM.32 Furthermore, Safranal showed pro-apoptotic effects in HepG2 cells, activating intrinsic and extrinsic caspases and promoting cell death through endoplasmic reticulum (ER) stress.32 It reduced HUVEC growth (IC50 = 300 μM) and blocked VEGF release in HepG2 cells, indicating potential anti-angiogenic effects.33 Furthermore, Safranal prevented endothelial cell migration and tube formation, supporting its anti-angiogenic properties.33 These findings highlight Safranal's various effects on liver cancer cells and its potential as a valuable therapeutic agent. However, stability and bioavailability limitations still hinder the clinical use of Safranal. It has been revealed that Safranal concentrations in mouse and rat plasma decrease significantly over time, highlighting this challenge.34 This study aims to investigate the intrinsic anticancer potential of MIL-88B(Fe) in combination with Safranal while considering the constraints of Safranal's stability and bioavailability.
Bacterial infections, on the other hand, remain among the leading causes of morbidity and mortality, posing a significant global public health risk. Antibiotic overuse contributes to the spread of antimicrobial resistance. The emergence and spread of antimicrobial resistance (AMR) results in the development of multidrug-resistant (MDR) bacteria, escalating global public health concerns.35 Nanoparticles (NPs) are usually used in antibiotic delivery systems, bacterial detection systems for microbial diagnostics, and antibacterial vaccines to control bacterial infections. While the precise mechanisms of NPs’ antibacterial action are unknown, established possibilities include promoting oxidative stress, metal ion release, and non-oxidative routes.36 In the past few years, MOFs have gained significant attention for diverse antibacterial applications due to their antibacterial capabilities resulting from different physical and chemical features. These include metal ion or organic compound controlled release and enzyme-like, photocatalytic, and photothermal activity.37
This work aims to overcome Safranal's limitations by incorporating it into/onto the MIL-88B(Fe) structure, paving the way for natural products to emerge as effective medicines in the treatment of liver cancer. The study also investigates MIL-88B(Fe)'s promising antibacterial characteristics and potential as a dual-purpose therapeutic agent for cancer and bacterial infections. This research adds to the growing understanding of using Fe-MOFs in biomedicine. It demonstrates the potential of safranal-loaded MIL-88B(Fe) as a diverse and practical treatment approach.
For the evaluation of the anticancer characteristics of the MIL-88B(Fe) and the SAF@MIL-88B(Fe) nanostructures, the following chemicals and reagents were used: antibiotic–antimycotic solution for cell culture – A5955, fetal bovine serum (10%), 3-[4,5-dimethylthiazol-2-yl]-2,5-diphenyltetrazolium bromide (MTT), dimethyl sulfoxide (DMSO), and Dulbecco's phosphate buffered saline – Lot No. RNBL0732 were all obtained from Sigma-Aldrich. A HepG2 human liver carcinoma cells strain was obtained from ATCC (HB-8065), the cell culture media (RPMI 1640 Medium, with L-Glutamine) was obtained from Capricorn Scientific GmbH, Germany, a 0.25% trypsin solution was obtained from Cytiva, Marlborough, MA, USA, and a Mounting Medium containing 4′,6-diamidino-2-phenylindole (DAPI) (ab104139) was obtained from Abcam. In addition, a 4% paraformaldehyde was prepared in our laboratories.
For the evaluation of the antibacterial characteristics of the MIL-88B(Fe) and the SAF@MIL-88B(Fe) nanostructures, the following chemicals and reagents were used: E. coli strain obtained from the American Type Culture Collection (ATCC), Lactobacillus strain isolated from probiotic yogurt, LB Agar and LB Broth obtained from Lab M Limited, UK, Agarose obtained from Sigma-Aldrich, Bacterial Genomic DNA Isolation Kit (ab288102) obtained from Abcam, UK, RedSafe™ Nucleic Acid Staining Solution (20000×) obtained from iNtRON Biotechnology, South Korea, 1kb DNA Ladder obtained from Promega, and Gel Loading Dye Purple (6×) obtained from New England BioLabs.
To confirm the presence of Safranal in the MOF network, a solution of 0.7 mL dimethyl sulfoxide-d6 was added to 5 mg of MOF material. The resulting solution was heated until the powder completely dissolved. 1H NMR spectra were recorded at 25 °C in DMSO-d6 using a Varian-400 MHz instrument (USA), with solvent peaks at 2.50 ppm as internal references. The assignment of chemical shifts was relative to a known standard Safranal.
The release of Fe3+ ions and Safranal from the pure and Safranal-loaded MIL-88B(Fe) nanostructures was monitored using ICP-MS and UV-VIS techniques, respectively. An inductively coupled plasma-mass spectroscopy (PERKIN ELMER ICP-MS, NEXION-2000G), USA used was for the follow up of release of Fe3+ ions. The release of Safranal was monitored using a UV-visible spectrophotometer. Fig. S1a (ESI†) shows a series of absorption spectra collected for different concentrations of safranal, where two main peaks were noticed at λmax values of 205 and 320 nm. A calibration curve was made for the peak at 205 nm, as shown in Fig. S1b (ESI†).
A 100 mL PBS solution containing MOF powder (at a concentration of 3 mg mL−1) was prepared in a conventional experimental setting. All samples were placed in a shaker incubator set at 100 rpm and 37 °C for up to 72 hours. Solution aliquots were collected at intervals of 0.5, 1, 6, 24, and 72 hours. To keep the volume consistent, fresh PBS was added after each 10 mL aliquot was removed. The collected solutions were filtered through a 0.2 μm syringe filter into separate vials and analyzed for [Fe3+] composition using the inductively coupled plasma-atomic emission spectroscopy (ICP-AES) technique. The experiment was repeated three times to ensure the reliability of the results.
To assess drug (Safranal) release, a 100 mL PBS solution containing SAF@MIL-88B(Fe) at a concentration of 3 mg mL−1 (inclusive of MIL-88B(Fe) + 7% Safranal) sample was prepared in a conventional experimental setting. All samples were placed in a shaker incubator set at 100 rpm and 37 °C for up to 144 hours. Solution aliquots were collected at intervals of 0.5, 1, 3, 6, 24, 48, 72, 96, 120, and 144 hours. After withdrawing 10 mL aliquots, fresh PBS was added each time an aliquot was removed to ensure a constant volume. The collected solutions were filtered through a 0.2 μm syringe filter into separate vials and analyzed using a UV-vis spectrophotometer. The experiment was repeated three times to ensure the reliability of the results.
Fig. 1 XRD pattern (a), FT-IR spectrum (b), TGA-DTG thermograms (c), and SEM micrographs (d) of the as-prepared MIL-88B(Fe) nanocrystals. |
Fig. 1(b) shows the FT-IR spectrum of the as-prepared MIL-88B(Fe). Three main features could be observed: bands at 1659.1, 1595.9, 1503.2, 1436.9, and 1390.3 cm−1 are attributed to the –OC–O− group, and bands at 748.5 and 1014.4 cm−1 are attributed to the C–H group of the terephthalate linker.36 The Fe–O absorption is shown at 554.9 cm−1, while the broad bands at 3423.1 cm−1 are related to the physically adsorbed water molecules.40Fig. 1(c) shows the TGA-DTG thermograms of the MIL-88B(Fe) nanostructure. The TGA thermogram starts with a slow rate of weight loss until 340 °C, which is attributed to the removal of weakly adsorbed volatile compounds, including water and/or organic solvents. This is followed by two thermal events, which were also confirmed by the DTG thermogram at 366.2 and 469.3 °C. These events amount to a weight loss of 35 and 71%, respectively. These events are related to the breakdown of the MOF structure at 366.2 °C, followed by a complete decomposition of the organic content of the MOF at 469.3 °C. An iron oxide residue is formed after 600 °C after complete decomposition of the MOF structure.
Fig. 1(d) shows the morphology of the as-prepared MIL-88B(Fe) nanostructures. A homogeneous particle size distribution of the MIL-88B(Fe) diamond-shaped crystals can be observed. The inset of the SEM micrograph shows a sharp-edged diamond-shaped MIL-88B(Fe) crystal with an average length of 600 nm and width of 500 nm. These findings confirm the phase purity and morphology of the synthesized MIL-88B(Fe) nanocrystals. Fig. S2 (ESI†) shows the N2-adsorption–desorption hysteresis of the as-prepared MIL-88B(Fe) nanostructure, where the nanostructure exhibited a type III isotherm with a BET surface area of 4.9 m2 g−1. This low surface area could be related to the breathing characteristic of the MIL-88B nanostructure, which is known to exhibit variable (low-to-high) surface area depending on reaction conditions.39
The effect of loading MIL-88B(Fe) with different percentages of Safranal on the structure and morphology of the formed SAF@MIL-88B(Fe) composite nanostructures is shown in Fig. 2–4. Fig. 2(a) shows the XRD patterns of the SAF@MIL-88B(Fe) nanostructures, where a consistent stability of the phase composition of the MIL-88B(Fe) structure was observed by increasing the concentration of SAF. All XRD peaks in the patterns of the SAF@MIL-88B(Fe) nanostructures were indexed with those shown in the XRD pattern of the pure MIL-88B(Fe). However, an additional peak was observed at 8.73° with increasing intensity upon increased SAF content. The presence of this peak could be related to the inclusion of the SAF molecule within the intrinsic porosity of the MIL-88B(Fe). The presence of Safranal in the SAF@MIL-88B(Fe) nanostructures was further confirmed by FTIR and TGA-DTG analyses. Fig. 2(b) shows the FTIR spectra of the SAF@MIL-88B(Fe) as compared with that of pure MIL-88B(Fe). All spectra confirmed the structure MIL-88B(Fe). In addition, two low-intensity bands were observed at 2870 and 2968 cm−1, and an additional band was observed at 679 cm−1. These bands refer to the absorption of the C–H (of CH3) and –CO (of –CHO) of Safranal. These bands are identified in the FTIR spectrum of pure Safranal oil shown in Fig. S3 (ESI†).
Fig. 2 XRD pattern (a), FT-IR spectra (b), TGA (c), and DTG (d) thermograms of pure MIL-88(Fe) and SAF@MIL-88(Fe) nanostructures containing 3, 5, 7, and 10% SAF. Arrows in Fig. 2(b) refer to the presence of safranal in the SAF@MIL-88 nanostructures. |
Fig. 2(c) shows the TGA thermograms of the SAF@MIL-88B(Fe) composite nanostructures. Compared with the two main thermal events of the SAF-free MIL-88B(Fe), as shown in Fig. 1(c), all TGA thermograms of the composite nanostructures showed multiple thermal events. This was further confirmed in the DTG thermograms of the composite nanostructures in Fig. 2(d). The multiple thermal events are summarized in Table 1. The first thermal event was observed in the range of 34–55 °C, and the second thermal event was observed in the range of 155–200 °C, both with increasing intensity with the increase of the safranal content. These events amount to an overall weight loss of 40%. These events could be related to the removal of the weakly adsorbed solvent and safranal molecules. These events were followed by a more shallow thermal event within the range of 349–367 °C with a shift towards lower temperature upon the increase of the safranal content. This event was followed by a more pronounced thermal event within the range of 432–470 °C with the same trend of increasing intensity upon increasing the safranal content. The third thermal event within the range of 349–367 °C could be attributed to the breakdown of the MOF structure, and the variation in the average temperature of its occurrence could be related to the presence of the more volatile, chemically bonded safranal molecules within the porosity of the MOF nanostructure. The fourth thermal event within the range of 432–470 °C could be attributed to the decomposition of the organic content of the nanostructures, and the increased intensities of these events with increasing the safranal content could be related to the presence of safranal-linker and/or safranal-coordinated Fe–O clusters within the structure. The last thermal event was observed within the range of 469–490 °C. It could be related to the decomposition of Safranal-coordinated Fe–O clusters, which is confirmed by its occurrence in the SAF@MIL-88B(Fe) thermograms and its absence in the thermogram of the pure MIL-88B(Fe) nanostructure.
[SAF] (%) | Thermal events – peak temperatures | ||||
---|---|---|---|---|---|
0 | 53.6 | None | 366.3 | 432.5 | 469.5 |
3 | 45.1 | 176.3 | 364.1 | 469.0 | 488.4 |
5 | 45.1 | 194.5 | 342.9 | 448.4 | 489.6 |
7 | 34.8 | 179.7 | 342.9 | 448.4 | 489.6 |
10 | 39.9 | 156.9 | 349.7 | 448.4 | 489.6 |
It should be mentioned that the analysis of the aliquots produced, after suspending MIL-88B(Fe) in the SAF solutions containing 3, 5, 7, and 10% of SAF, using UV-vis confirmed the complete incorporation of SAF within the MIL-88B(Fe) structure. No signs of remaining SAF were observed in these aliquots. Based on the breathing effect of MIL-88B(Fe), it is known that MIL-88B(Fe) mostly adopts the closed structure while in the solid state, and opens up its porosity when in solution.6,7 It is, therefore, believed that the incorporation of SAF in the MIL-88B(Fe) structure in solution takes place within the temporarily open porosity of the MIL-88B(Fe) when mixed in PBS media, as well as immobilized onto the external surfaces of the MIL-88B(Fe) structure through potential H-bonding formation. Fig. S4 (ESI†) shows a schematic representation of the interaction between a Safranal molecule within the pore and onto the surface of a MIL-88B(Fe) structure. Considering an average pore size of 62 nm of the open structure of MIL-88B(Fe) and an average size of 8 nm of a typical Safranal molecule, it is apparent that safranal molecules can be entrapped within the open pores of the MIL-88B(Fe) in solution in addition to adsorption on the external surfaces of the MIL-88B(Fe) nanostructure. The interaction between the Safranal molecules in both cases is believed to take place through H-bonding and coordination bonding formation, as indicated in Fig. S4 (ESI†).
The presence of Safranal within the nanostructure of the MIL-88B(Fe) was further confirmed by 1H NMR, as shown in Fig. 3, as a function of the loading of Safranal in the nanostructure. The absence or poor appearance of hydrogen nuclear magnetic resonance (H-NMR) signals for SAF@MIL-88B(Fe) composite nanostructures can be attributed to many iron complexes being paramagnetic due to the presence of unpaired electrons in the d orbitals of the iron ion. On the other hand, the continued presence of a broad peak at a chemical shift of 1.2 ppm with increasing the safranal contents is an indication of the 1H of the 2 CH3 groups along the structure of the safranal molecule. The peak broadening observed in the spectra of the SAF@MIL-88B(Fe) composite nanostructures could be attributed to the paramagnetic characteristics of the iron complex structure. As a result, signals from individual protons become less resolved and may merge into a broad hump or baseline, making it challenging to assign peaks to their corresponding protons. Both DMSO and Water were shown as sharp peaks at 2.1 and 3.3 ppm, respectively. These peaks were also observed with more broadening in the NMR spectra of the SAF@MIL-88B(Fe) composite nanostructures.
To confirm the presence of the 1H of the 2 CH3 groups along the safranal molecule in the SAF@MIL-88B(Fe) as compared with the peaks of the solvents (DMOS and H2O) used, a composite nanostructure containing the highest loading of safranal (10%) was titrated against deuterated HCl (DCl), as shown in Fig. S5 (ESI†). The peaks at 1.2 and 2.1 ppm, attributed to the 1H of the safranal 2CH3 groups and the DMSO solvent, were continuously present in the spectra of all samples upon increasing the volume of DCl. On the other hand, the peak at 3.3, which is attributed to 1H of water, was observed to shift towards higher chemical shifts with increasing the volume of DCl. To further confirm this finding, a similar titration experiment was conducted for pure safranal, where the 1H of water peak at 3.3 was shifted to higher chemical shifts with increasing the volume of DCl, as shown in Fig. S6 (ESI†). These findings further confirm the presence of safranal within the MIL-88B(Fe) nanostructure.
The effect of including safranal within the MIL-88B(Fe) nanostructure on the morphology of the produced crystals was examined using SEM microscopy, as shown in Fig. 4. The diamond-shape morphology of the MIL-88B(Fe) crystals was maintained with increasing the safranal loading. However, a slight deformation of the MIL-88B(Fe) crystals was observed, especially at higher safranal loadings. With reference to the XRD patterns of these samples (Fig. 2(a)), the phase composition and crystallinity of the MIL-88B(Fe) nanostructures were maintained despite the observed variations in the surfaces of these nanostructures.
Fig. 4 SEM micrographs of SAF@MIL-88B(Fe) nanostructures containing (a) 3, (b) 5, (c) 7, and (d) 10% SAF. |
Fig. 5 XRD patterns of MIL-88B(Fe)(a), (b) and SAF7@MIL-88B(Fe) (c), (d) after incubation in PBS (a), (c) and RPMI (b), (d) media for 0, 24, 48 and 72 hours at 37 °C. |
Fig. 6 SEM micrographs of MIL-88B(Fe) (a)–(f) and SAF7@MIL-88B(Fe) (g)–(l) after incubation in PBS (a)–(c) and (g)–(i) and RPMI (d)–(f) and (j)–(l) media for 24, 48 and 72 hours at 37 °C. |
The effect of treatment of both MIL-88B(Fe) and SAF7@MIL-88B(Fe) nanostructures with RPMI media was also reflected in their composition and morphology, as shown in Fig. 5 and 6. A gradual degradation of the MIL-88B(Fe) nanostructure in RPMI was also observed to take place with time, as shown in Fig. 5(b), which was also reflected in the morphology of the RPMI-treated MIL-88B(Fe) crystals (Fig. 6(d)–(f)). A similar pattern was observed for the SAF7@MIL-88B(Fe) crystals after immersion in RPMI media for up to 72 hours, where a gradual decrease in the crystallinity of the nanostructures was noticed (Fig. 5(d)). This was also accompanied by a visual decline in the sharpness of the SAF7@MIL-88B(Fe) crystals’ morphology (Fig. 6(j)–(l)). The degradation of the MIL-88B and SAF7@MIL-88B(Fe) nanostructures in PBS and RPMI media indicate their potential to degrade in vitro, hence releasing both Fe3+ ions and safranal with time in vitro.
The kinetics of release of Fe3+ ions and safranal from the MIL-88B(Fe) and SAF7@MIL-88B(Fe) nanostructures was monitored as a function of time. Fig. 7(a) shows a sudden release of Fe3+ ions from MIL-88B(Fe) and SAF7@MIL-88B(Fe) nanostructures within the first 60 minutes of immersion in PBS media. The extent of release of Fe3+ ions was more pronounced in the case of SAF7@MIL-88B(Fe) than that of pure MIL-88B(Fe). Both nanostructures showed a decrease in the concentration of Fe3+ ions in solution within a course of 24 hours. The release of Fe3+ ions from the MIL-88B(Fe) and SAF7@MIL-88B(Fe) nanostructures ceased after 7 and 24 hours, respectively, followed by a minimal release throughout the experiment (up to 72 hours). These results agree with the XRD results shown in Fig. 5(a), where the formation of iron(III) phosphate was observed in the XRD pattern of the 24 hours-treated MIL-88B(Fe) sample. This indicates that the formation of the iron(III) phosphate structure is a product of the transformation of the MOF structure. The higher extent of release of Fe3+ ions from the SAF7@MIL-88B(Fe) indicates the possibility of chemical interaction between the safranal molecules and the Fe3+ clusters in the MIL-88B(Fe) MOF structure, which is confirmed by the release of safranal from the SAF7@MIL-88B(Fe) nanostructure within the same timeframe (Fig. 7(b)). The release of safranal from the SAF7@MIL-88B(Fe) nanostructure in Fig. 7(b) shows a 2-phase release pattern. An initial burst is observed within the first 30 minutes (25.17 μg mL−1) from SAF@MIL-88B(Fe), which is believed to be attributed to the detachment of the weakly adsorbed safranal molecules. This is followed by a second stage of sustained release of safranal reaching 28.0 μg mL−1 after 72 hours of immersion in PBS media.
It should be mentioned that safranal exhibits strong absorption in the 200–400 nm range with two distinct peaks at around 205 and 320 nm, attributed to the π–π* and n–π* transitions, respectively.42 During the release study of safranal from the SAF7@MIL-88B(Fe) in PBS medium, the absorption at 205 nm only was observed, while the signal at 320 nm was absent (Fig. S1, ESI†). The absence of absorption at 320 nm, characteristic of safranal's n–π* transition, suggests that this particular molecular state or interaction was altered or disrupted. It is, therefore, considered a further confirmation of the interaction between the safranal molecule and MIL-88B(Fe) MOF structure, resulting in a change in the safranal's microenvironment leading to the disappearance of the n–π* transition at 320 nm.
The sustained release of safranal is likely attributed to the gradual diffusion of safranal molecules trapped within the MOF's porous structure. The pore size, surface properties, and interactions between MIL-88B(Fe) nanostructure and safranal molecules govern the diffusion rate, resulting in a controlled and prolonged release. This biphasic profile suggests potential advantages for using safranal therapeutically. The initial burst may have a faster therapeutic effect, which could be helpful for acute conditions that require prompt action. The sustained release ensures that safranal remains in the body for an extended time, potentially boosting overall therapy efficacy and reducing dose frequency, which can increase patient compliance. Furthermore, depending on the MOF design, the controlled release may allow the targeting of specific tissues or organs, reducing the possibility of side effects on healthy tissues.
In this regard, pure MIL-88B(Fe) and that loaded with 7% safranal (SAF7@MIL-88B(Fe)) were evaluated for their cytotoxic effects against HepG2 liver cancer cells following 24 and 48-hour incubation periods. Fig. 8 and 9 depict the trend in cell viability of MIL-88B(Fe) and SAF7@MIL-88B(Fe), respectively, after 24 and 48 hours of incubation at 37 °C. Results indicate that both materials exhibit a dose-dependent effect on HepG2 cells. After 24 hours of incubation, MIL-88B(Fe) inhibited 50% of cells at 11.770 μg mL−1 (Fig. 8(a)), while SAF@MIL-88B(Fe) inhibited 50% of cells at 9.510 μg mL−1 (Fig. 9(a)). After 48 hours of exposure, cell viability reduced significantly, with IC50s of 6.372 μg mL−1 (Fig. 8(b)) and 3.459 μg mL−1 (Fig. 9(b)) for MIL-88B(Fe) and SAF@MIL-88B(Fe), respectively. These findings indicate that both materials considerably influence the metabolic activity of HepG2 cells. Moreover, the values suggest a potential synergistic effect of MIL-88B(Fe) and safranal.
Nuclear morphology evaluation was carried out using DAPI staining, where DAPI (4′,6-diamidino-2-phenylindole) is a fluorescent dye that binds particularly to adenine–thymine (AT)-rich DNA segments, allowing cell nuclei to be visualized.43 Following DAPI staining and fluorescence microscopy imaging, shown in Fig. 8(c) and 9(c), the observed nuclear morphology supports that MIL-88B(Fe) and SAF@MIL-88B(Fe) support the assumption of a dose-dependent effect on the treated cells. As the MOF concentration increased, apparent alterations in nuclear morphology were observed, including variations in size, shape, and intensity.
The dose-dependent pattern is more visible when the MOF concentration increases from lower to higher levels. Normal nuclei with uniform DAPI staining at lower doses were more prevalent; however, there was an apparent rise in condensed or fragmented nuclei at higher concentrations, indicating a potential trigger for cellular stress or apoptotic processes. These findings suggest narrowing the dose selection to 2.5–25 μg mL−1 for further investigation of the MOFs’ impact on HepG2 cells. Future studies will utilize cellular assays and molecular analysis to investigate the mechanisms underlying this dose-dependent response.
The minimum inhibitory concentration (MIC) for MIL-88B(Fe) and SAF@MIL-88B(Fe) nanostructures against E. coli and Lactobacillus at various concentrations (7.81–2000 μg) was carried out, as shown in Fig. S8 and S9 (ESI†). Following a 16-hour treatment period, both MOF nanostructures had inhibitory effects against bacterial strains at the maximum concentration tested at 2000 μg (Tables S1 and S2, ESI†). Furthermore, MIL-88B(Fe) and SAF@MIL-88B(Fe) displayed partial inhibition at a concentration of 1000 μg. These results show the antibacterial activity of both Fe-MOFs against E. coli and Lactobacillus, with the same levels of inhibition observed at different concentrations.
The mechanism of antimicrobial activity of both types of MOF nanostructures was analyzed by the DNA disintegration method, which indicates the inhibition of nucleic acid synthesis while incubating microorganisms in the presence of MOFs, as shown in Fig. 10(c)–(f). MIL-88B(Fe) achieved total degradation on E. coli as observed in lanes 3, 4, and 5 (0.5, 1, and 1.5 times the MIC) (Fig. 10(c)). The spectrum of the impact caused by SAF@MIL-88B(Fe) on E. coli is shown in Fig. 10(d), with partial degradation observed in lanes 1–3 (0.125, 0.25, and 0.5 times the MIC) and total degradation in lanes 4 and 5 (1 and 1.5 times the MIC). Results are also summarized in Tables S3 and S4 (ESI†) using a Nanodrop 2000 (Thermo Fisher). The data shown in Table S3 (ESI†) show a decrease in DNA concentration as the concentration of MIL-88B(Fe) increased. This is consistent with the observation that MIL-88B(Fe) effectively degrades E. coli DNA. Furthermore, Table S4 (ESI†) presents the DNA quantification of E. coli treated with SAF@MIL-88B(Fe). Similar to MIL-88B(Fe), SAF@MIL-88B(Fe) demonstrates a dose-dependent effect on DNA degradation. As the SAF@MIL-88B(Fe) concentration increased, the DNA concentration progressively decreased. This observation aligns with the findings from Fig. 10(c) and (d), which visually depicted partial degradation at lower concentrations and complete degradation at higher concentrations of both MOF nanostructures.
The agarose gel electrophoresis of both MIL-88B(Fe) and SAF@MIL-88B(Fe) caused complete degradation of Lactobacillus DNA across a concentration range ranging from 0.125 to 1.5 times the MIC. Fig. 10(e) and (f) visually demonstrate this genotoxic effect, respectively. Table S5 (ESI†) explores Lactobacillus treated with MIL-88B(Fe) and indicates a dose-dependent decline in DNA concentration. All concentrations tested showed a significant and notable reduction in DNA concentration, aligning with the complete degradation observed in Fig. 10(e). Table S6 (ESI†) examines Lactobacillus treated with SAF@MIL-88B(Fe), also displaying a dose-dependent decrease in DNA concentration, aligning with the complete degradation observed in Fig. 10(f). These DNA quantification tables provide quantitative evidence supporting the visual observations from the figures, solidifying the conclusion that both MIL-88B(Fe) and SAF@MIL-88B(Fe) MOF nanostructures are effective antibacterial agents against E. coli with a pronounced efficacy against Lactobacillus.
Scheme 2 Mechanism of action showing the anticancer (a) and antibacterial (b) capabilities of the SAF@MIL-88B(Fe) nanostructures. |
These Fe2+ ions participate in Fenton-like reactions with hydrogen peroxide, generating highly reactive hydroxyl radicals that can induce lipid peroxidation and oxidative stress, ultimately leading to ferroptosis—a specific form of cell death in cancer cells. Simultaneously, safranal within MIL-88B(Fe) contributes to the inhibition of cell proliferation of HepG2 cells, enhancing the cytotoxic effect of the nanoparticles. This action of MIL-88B(Fe) and safranal presents a potential strategy for targeted liver cancer therapy. On the antibacterial front, MIL-88B(Fe) nanoparticles release Fe2+ ions in the bacterial environment. These ions, along with safranal, can disrupt bacterial cell membranes, leading to damage to cellular components and DNA, ultimately resulting in bacterial death. This highlights the importance of future research to validate the proposed mechanism of action and optimize the therapeutic potential of MIL-88B(Fe) loaded with safranal against both liver cancer and bacterial infections.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ma00345d |
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