Open Access Article
Alessio
Zuliani
*,
M.
Carmen Castillejos
and
Noureddine
Khiar
*
Asymmetric Synthesis and Nanosystem Group (Art&Fun), Institute for Chemical Research (IIQ), CSIC-University of Seville, 41092 Sevilla, Spain. E-mail: a.zuliani@csic.es; khiar@iiq.csic.es
First published on 21st November 2023
Zirconium-based MOFs, such as PCN-222 (MOF-545), have gained attention due to their regular porosity, tuneable pore size, versatile structure and exceptional thermal/chemical stability. However, the synthesis of PCN-222 using traditional batch processes suffers from limitations in productivity, scalability, and control over size and morphology. This study presents a paradigm shift from batch to continuous flow (c.f.) synthesis for the efficient production of PCN-222. The optimization of batch conditions and exploration of c.f. parameters enabled the synthesis of high-quality PCN-222 with Space–Time–Yield (STY) exceeding 950 kg m−3 day−1. The c.f. approach offered advantages including improved resource efficiency, safer chemical handling, and scalability. The integration of ultrasound-assisted technique into the c.f. facilitated the shaping of PCN-222 into prolate ellipsoids, making it suitable for applications in drug delivery and catalysis. The successful substitution of hazardous solvents with greener alternatives further enhanced the sustainability of the process. Finally, the loading of a thio-N-acetylgalactosamine-PEG-sulfate ligand on PCN-222 in tandem c.f., expanded the potentialities of the flow synthetic approach. This study not only advances the field of MOF synthesis but also paves the way for efficient and sustainable manufacturing processes in c.f. synthesis of nanoparticles and functionalized nanoparticles for active drug delivery.
000 different MOFs have been explored for potential applications in drug delivery, imaging, sensing, catalysis, gas (hydrogen, carbon dioxide, methane) storage and other biomedical uses, and a further half a million structures of MOFs have been hypothesized.3
Among all, zirconium (Zr) based MOFs are gaining prominence due to their unique combination of properties. For instance, Zr-based MOFs have exceptional thermal and chemical stability, making them ideal for high-temperature applications and in harsh chemical environments. In addition, the Zr metal center has a high coordination number and large ionic radius, which can lead to a diverse range of structures by supporting a large variety of organic ligands. A Zr-based MOF having attracted attention in the last decade is the porous coordination network-222 (PCN-222, also known as MOF-545), firstly synthesized in 2012.4–6 PCN-222 is composed of Zr(IV) clusters connected by tetrakis(4-carboxyphenyl)porphyrin (TCPP) ligands through Zr–carboxyl bonds in a three-dimensional porous network structure. The strong coordination bond between Zr and O, rising from the high charge density and bond polarization of the highly oxidated Zr(IV), results in a highly robust structure. The morphology of PCN-222 is mainly reported as micro-dimensional (>1 μm length) needle/rod-shaped crystals or, less frequently, as prolate ellipsoids (ranging from ca. 50 nm up to more than 500 nm), while the strict control of the size-distribution of PCN-222 is hardly achieved.7,8 The main characteristics of PCN-222 include high surface area of up to more than 2000 m2 g−1 and large pore volume. Thus, PCN-222 has been mainly explored for storing gases such as methane, hydrogen, and carbon dioxide and as a catalyst in organic transformations and in the immobilization of enzymes. Concerning the field of biomedicine, PCN-222 has recently attracted considerable attention due to its remarkable acid stability and biocompatibility, which offer the potential for targeted drug delivery to specific sites such as acidic tumour environments. Moreover, PCN-222 can be used as pH-sensitive drug delivery system, further enhancing its therapeutic applications.9 Additionally, PCN-222 finds potential utility in photodynamic therapy (PDT) when exposed to laser irradiation.10 The captivating biomedical applications of PCN-222 are underscored by the prospect of drug-loaded PCN-222 possessing substantial commercial value, offering opportunities for cost-effective production methods. This contrasts with other applications, such as gas storage or catalysis, where achieving economic viability can be more challenging. For example, Fairen-Jimenez et al. loaded a model drug (doxorubicin) on PCN-222 PEGylated with PEG-phosphate ligands forming a composite having excellent water dispersibility at room temperature, improved colloidal stability and delayed drug-release kinetics of the drug.11 Notwithstanding the potential of PCN-222, its synthesis has only been performed using batch processes, which can suffer from several limitations such as low yields and productivity, long reaction times, and difficulty in scaling up. Typically, the solvothermal synthesis of PCN-222 is performed under laboratory conditions by dissolving a Zr-precursor (normally Zr chloride or previously synthesised Zr6 clusters), TCPP and an acid modulator (usually benzoic acid, trifluoroacetic acid or fluorobenzyl acid) in N,N-dimethylformamide (DMF), followed by heating at 393 K under magnetic stirring from a few up to 48 hours.12–14 The purification of the so-synthesized PCN-222 is performed by centrifugation. The slow crystallization rate of PCN-222 together with heat and mass transfer issues limits the scale up of the process, restricting the production to a few mg per batch. Furthermore, the use of high volume of hazardous DMF entails important limits especially considering health and environmental issues.15 Therefore, the design of more efficient, sustainable, and scalable synthetic methods based on alternative techniques such as mechanochemistry, microwave chemistry, ultrasound-assisted synthesis and continuous flow synthesis is crucial to overpass these inefficiencies and to perform accessible production of PCN-222. The first effort for the scalable synthesis of PCN-222 reported up to date exploited microwave chemistry to produce tens of mg of the MOF with yields of 72%, within only 30 minutes.16 However, the poor control on the morphology and on the size-distribution of the MOF cannot be applied for many applications, such as drug delivery, where nanosystems must have controlled size and morphology to regulate their circulation and clearance kinetics in the bloodstream. Indeed, it has been demonstrated that specific shapes, such as prolate ellipsoidal nanoparticles exhibit lower rates of systemic elimination compared to particles with other shapes, indicating that they may circulate in the bloodstream for longer periods.17 In addition, the smaller particle size shows long in vivo circulation time, although this should be carefully checked also considering the hydrodynamic size in the blood stream. Another example for the scalable synthesis of PCN-222 has been recently reported by Yu et al. through an ultrasound-assisted method. In details, the researchers were able to synthesize PCN-222 in high crystal purity and uniform size within 30 minutes.18 Still, the use of batch synthesis limits the potential scale up of the synthesis, with important sustainable drawbacks, including low energy efficiency and high chemical risk.
In the past few years, continuous flow (c.f.) chemistry has emerged as an attractive alternative to batch synthesis methods for the efficient preparation of different chemicals and materials and has been pointed out as promising path for the industrialization of MOFs.19 C.f. chemistry offers several advantages over batch processes including resource efficiency, reduced waste generation, safer chemical handling, energy efficient, scalability and process intensification.20,21 C.f. has been also reported by the IUPAC as one of the “Top Ten Emerging Technologies” with the potential to turn the planet more sustainable.22 Furthermore, external fields such as microwave or ultrasound (US)23 can be coupled to c.f. to enhance heat transfer, facilitate the disruption of agglomerates of particles, boost the mix of the reagents and precursors in the channel and reduce the undesired deposition of solid materials on the channel wall. At the same time, US have been proved to have multiple effects such as accelerating the nucleation and growth to get monodispersed nanoparticles, influencing the crystal morphology and etching the crystals.18,24
Here, the first use of a c.f. reactor for the synthesis of PCN-222 with defined and sized-controlled prolate ellipsoid morphology (down to less than 100 nm) is reported. After optimizing the batch conditions in terms of ligand-to-metal cluster molar ratio (0.3–2.5), sequential experiments in c.f. examined the influence of ligand concentration (3.2–7.1 mM), flow rate (0.1–5 mL min−1), ligand-to-acid modulator molar ratio (0.007–0.054) and temperature (383–418 K). Considerations of some specific parameters on the sustainability of the synthesis were determined by the green metrics Environmental factor (E-factor) and Reaction Mass Efficiency (RME). The best reaction conditions allowed overpassing the challenge of preserving the quality of MOF during the rapid synthesis in c.f. The c.f. method was thus combined with US technique (20 kHz, 20–90% US amplitude) allowing the etching of the crystals and the shaping the MOF into prolate ellipsoids by variations of the dimensions of the minor axis (i.e., the equatorial axis) of the ellipsoids. Greener alternative solvents to hazardous DMF were also evaluated. The c.f. synthesis yielded high-quality PCN-222 with Space–Time–Yield (STY, one of the most common parameters representing the productivity of the synthesis) up to more than 950 kg m−3 day−1, demonstrating the robustness and scalability of the method. The potential biomedical applications of PCN-222 were finally evaluated by the loading a thio-N-acetylgalactosamine-PEG-sulfate ligand (S-GalNAc-PEG-sulfate) in tandem c.f. The ligand was incorporated onto the PCN-222 particles through Zr–sulfate interactions, contributing to the stabilization of the PCN-222 particles. Additionally, the incorporation of thio-N-acetylgalactosamine (S-GalNAc), a glycosidase-resistant analogue of natural GalNAc, holds great promise as it specifically targets the asialoglycoprotein receptor (ASGPR) overexpressed on hepatic cancer cells. This presents an exciting opportunity to efficiently develop a porphyrin-based drug delivery system using continuous flow synthesis.
000 rpm, 15 min), washed one time with DMF, and exchanged two times with ethanol (EtOH).
Firstly, commercially available N-acetylgalactosamine tetra-acetate 1 was treated with Lawesson's Reagent in toluene at 353 K to provide the cyclized per-O-acetylated thiazoline 2 with 71% yield. The heterocycle in compound 2 was subsequently cleaved through acid hydrolysis using TFA and water in methanol (MeOH) at 273 K.27 This process resulted in the production of thiol 3 with an 85% yield. Secondly, octaetyleneglycol 4 was treated with SOCl2 in the presence of 4-dimethylaminopyridine (DMAP) and diisopropylethylamine (DIPEA) in dichloromethane (DCM) from 273 K to r.t., affording cyclic sulfite 5 with 91% yield. Subsequently, the oxidation of 5 was carried out using NaIO4 with a Ru-catalyst in a mixture of acetonitrile (I), trichloromethane (TCM), and water, resulting in the formation of cyclic sulfate 6 with a yield of 79%.28 The condensation of thiol 3 with cyclic sulfate 6, using triethylamine (Et3N) as a base in dimethylformamide (DMF) at r.t., resulted in the formation of compound 7 with a yield of 61%. Lastly, compound 8, i.e., the S-GalNAc-PEG-sulfate ligand, was obtained in quantitative yield though Zemplen deacetylation of 7, carried out using MeONa in MeOH at r.t. Details of the synthesis as well as 1H-NMR, 13C-NMR and mass spectroscopy of the compounds are reported in the ESI.†
000 rpm for 15′ followed by one wash in DMF and two wash in EtOH. Details of the chemicals and of the characterization techniques are reported in ESI section-S2.†
In order to evaluate the productivity of the synthesis in c.f., the Space–Time–Yield (STY)29 was calculated according to eqn (1):
![]() | (1) |
Each experiment was repeated at least three times in order to determine the STY, which was thus reported with its corresponding standard deviation.
![]() | (2) |
![]() | (3) |
The metrics were calculated using the mean mass of the synthesized PCN-222 obtained in the different runs of each experiment. As easily understandable, the lower the E-factor the lower the environmental impact of the synthesis. For example, the general E-factor found in different industrial segments varies form ca. 0.1 of oil refining, to 1–50 of fine chemicals and 50–100 of pharmaceuticals.26 On the contrary, the higher the RME, the lower the environmental impact of the synthesis. In the present study, to accentuate the disparity between batch and c.f. synthesis, green metrics were discussed without accounting for solvents. This omission was supported by the ease with which solvents can be recycled after separation from PCN-222, typically through centrifugation, rendering them potentially non-waste materials.26 Green metrics were calculated using the average mass of PCN-222 produced in each experiment. For instance, in an experiment (entry 4 in Tables S2 and S3 in the ESI†), 11.5 mg of PCN-222 (STY: 5.5 kg m−3 day−1) was produced using 22.5 mg of TCPP, 33.0 mg of Zr6 nodes, and 193.7 mg of TFA (130 μL), totalling 249.2 mg of mass of reagents (excluding the solvent used in the reaction, DMF, and the solvents for washing, DMF and EtOH). The waste mass was determined by subtracting the mass of the product and corresponded to 237.7. Thus, the E-factor was 20.7 (calculated as 237.7 divided by 11.5), and the RME was 4.6% (calculated as 11.5 divided by 249.2 and multiplied by 100). To provide a comprehensive overview, the E-factor calculated considering also the solvents can be checked in the ESI (RME does not count solvents).†
:
M) as well as the concentration of reactants and amount of acid modulator, merely focusing on the reaction STY without considering the size-distribution of the produced particles (ESI Table S1†). Reaction time was not considered to be optimized in this phase since the reactions in c.f. were sequentially always carried out in much less than 5 h. The preliminary tests highlighted that the L
:
M was the most relevant parameter with effect on the reaction STY. As a result, a sequence of batch experiments was performed to investigate the influence of the L
:
M on the STY, the length of the particles, and the size-distribution of PCN-222 (ESI Table S2†), as summarized in Fig. 3.
![]() | ||
Fig. 3 (a) Variation of L : M vs. STY and size of the obtained PCN-222 particles. Reaction conditions: 393 K, 5 h, 22.5 mg TCPP (0.0284 mmol, 3.55 mM), 8 mL DMF, 130 μL TFA (L : Mod 0.017). (b) SEM images of PCN-222 obtained using L : M of 1 and L : M of 0.3, respectively, highlighting the changes in particle-size distribution in function of the amount of Zr6 clusters used. See ESI section-S3† for additional SEM images. | ||
In all the experiments, the concentration of the ligand TCPP was kept constant, while the quantity of Zr6 nodes was varied to tune the L
:
M from 0.3 to 2.5 (see ESI section-S3†).
Considering that the molecular formula of PCN-222 is Zr6(μ3-OH)4(μ3-O)4(C48H26N4O8)2, formed by TCPP4− ligand (C48H26N4O8) and Zr6(μ3-OH)4(μ3-O)4 nodes34 the results showed that, to increase the STY of PCN-222, it was necessary to use less quantity than the (theoretical) stoichiometric amount of the ligand TCPP (i.e., more Zr6 clusters). This was particularly evident when the L
:
M was equal or less than 1. At the same time, the size of the PCN-222 was observed to increase when more quantity of the metal clusters was used. This behaviour was in accordance with the reported literature related to other MOFs. In details, it is well established that a decrease of the ratio ligand–metal node influences (normally boosts) the nucleation and growth rates of MOF crystals, which in turn can also impact the size and the morphology of the final crystals.35,36 Thus, considering the STY of the synthesis, the best reaction conditions for the highest STY corresponded to the largest quantity of metal clusters. However, SEM images showed a substantial variation of the size-distribution of the PCN-222 when the L
:
M was ≤0.5. As a result, a L
:
M of 1 was selected for the shifting to c.f. synthesis, corresponding to the minimum quantity of Zr6 nodes required to obtain particles having sizes with relative SD of ca. 5% (222 ± 12 nm). A smaller L
:
M was discarded since it implied more consumption of metal nodes and, more importantly, larger SD (e.g., a L
:
M = 0.7 required 26% more metal nodes and resulted in a SD of ca. 10%). Importantly, the use of smaller L
:
M was also discarded considering no relevant variations in the green metrics of the synthesis. In details, when a L
:
M = 1 was used, E-factor = 20.7 and RME = 4.6%, while when L
:
M = 0.7, E-factor = 19.9 and RME = 4.8% (ESI Table S3†). The optimized batch conditions were thus selected for the shifting to c.f. synthesis. The importance of shifting the synthesis of MOFs to c.f. rises form the different benefits and advantages brought by this type of synthetic approach including improved control and reproducibility, enhanced reaction kinetics and product yield, safer and more controlled conditions, scalability, and production efficiency, reduced environmental impact, and finally versatility and process intensification. These advantages make the c.f. synthesis a promising approach to produce MOF with consistent quality and improved green characteristics and has been already applied in the synthesis of some types of MOFs such as UiO-66, MIL-100, and HKUST-1 (see ESI section-S4† for a detailed list of the most recent works related to the c.f. synthesis of MOFs). However, up to date, no report discusses the c.f. synthesis of the PCN-222/MOF-545.
![]() | (4) |
![]() | (5) |
The reaction was thus shifted to the c.f. system by mixing in a T valve two feeds, one with the ligand TCPP dissolved in DMF and the other with the Zr6 nodes and TFA dissolved in DMF. A T-valve was preferred to a cross-valve (where TFA would have been separated from the Zr6 clusters in another feed) since the Zr6 clusters did not completely dissolve in DMF without the presence of TFA (probably TFA substitutes the benzoate in capping the Zr6 nodes, making the nodes more polar, thus more soluble in DMF). The influence of the concentration of the reagents, the volumetric flow rate, the temperature of the reaction and the amount of employed acid modulator on the STY and on the size of the PCN-222 were thus singularly determined in c.f. Initially, the reaction was shifted to c.f. starting from the optimized batch conditions, which were 393 K reaction temperature, a L
:
M of 1, and a concentration of 3.6 mM TCPP, using DMF as solvent. According to the results of the preliminary tests, the amount of employed TFA was initially decreased (from a ligand-to-acid modulator molar ratio (L
:
Mod) of 0.017 to 0.027), aiming at diminishing the size of the particles11 and, more importantly, considering that the c.f. conditions do not imply the liquid–vapour equilibrium of TFA in the head space of the reactor observed in batch conditions (thus less acid was needed to obtain particles with the same dimensions of those obtained in batch). The amount of TFA used was then optimized after studying the effects of the volume of solvent, of the flow rate, and of the temperature.
:
M ratio, as shown in Fig. 4a. The lower limit of concentration was determined by too low STY (<50 kg m−3 day−1), while the upper limit was determined by the minimum amount of DMF needed to dissolve the reagents (in particular, TCPP).
The results demonstrated that the STY increased linearly with the concentration of the reagents. A similar behaviour was also observed concerning the size of the particles, but with a smaller slope (see ESI section-S6† for additional details and SEM images). Nevertheless, the size-distribution of the particles showed a SD ≤15% when the concentration of TCPP was ≤4.7 mM, while higher concentration implied bigger and more disperse particles. This was in accordance with the reported data in the literature concerning the synthesis of other MOFs, where it was observed that higher reagent concentration caused the less regularity of the shape and greater mean diameter.38 A concentration of 4.7 mM TCPP was thus selected for sequential experiments. Lower values of concentration were discarded since they implied more solvent consumption and substantially increased green metrics. In details, when an amount of solvent corresponding to a 4.7 mM concentration of TCPP was used, the E-factor and the RME corresponded to 61.7 and 1.6% respectively, which varied up to 190.8 and 0.5% respectively, when the concentration of TCPP corresponded to 3.2 mM (ESI Table S8†). This was attributed to the lower STY achieved when using a lower concentration of TCPP (implying less collision of particles, thus nucleation and crystal growth), while maintaining the same amount of Zr6 clusters and TFA.
![]() | (6) |
Note that the molecular formula here reported is slightly different from other formulas reported in the literature (e.g., Zr6(H2O)8O8(TCPP)2)6 due to utilization of previously synthesized Zr6 nodes capped with benzoate.11 Benzoate was substituted with TCPP during the synthesis, forming PCN-222. The moles of produced PCN-222, with molecular weight ca. 2253 g mol−1 and the moles of TCPP, with molecular weight 790.8 g mol−1, fed in the c.f. were thus calculated considering the volume of the reactor of 2.8 mL. For example, the experiment carried out at 0.5 ml min−1 flow rate, resulted in a STY of 161 ± 12 kg m−3 day−1, corresponding to 0.778 ± 0.058 × 10−3 mmol of PCN-222 (reaction time was 3.89 × 10−3 day). The mmol of TCPP fed in the system (4.7 mM) were 13.16 × 10−3, thus the TCPP conversion was 11.8 ± 0.9%. As shown in Fig. 4b, the conversion of TCPP diminished by diminishing the residence time (i.e., by increasing the flow rate), while the STY increased (Fig. S6 in the ESI† repots data in the 0.1–1 mL min−1 flow rate range). In details, by increasing the flow rate from 0.1 to 3 mL min−1, the STY passed from <50 kg m−3 day−1 up to >700 kg m−3 day−1. When the flow rate was between 3 and 5 mL min−1, the STY reached a plateau, since the faster flow was balanced by lower TCPP conversion. This meant that less MOFs were produced per mL of solution primarily due to the reduced time available for crystal growth, rather than for nucleation. This observation holds even when considering the small differences in the dimension of the particles. Higher flow rates were not considered since the conversion of TCPP at 5 mL min−1 was already too low (<6%). The observation of particle size in relation to flow rate was consistent with literature findings, showing that particle size increased linearly by increasing the flow rate up to 1 mL min−1. This phenomenon was attributed to higher flow velocities facilitating the advective transport of precursor species to nucleation sites in the flow, resulting in increased crystal growth rates and larger average crystal sizes, as seen for example in the c.f. synthesis of MOF-808.39 However, when the flow rate was further increased up to 5 mL min−1, the particle size was observed to slightly decrease, reaching almost a plateau with PCN-222 particles sizing ca. 87–97 nm length. This was explained by the shorter time available for crystallization (i.e., shorter τ), especially for crystal growth rate beyond nucleation rate, which resulted in smaller crystals. Additionally, the higher flow rate led to the competitive migration of precursor species to the nucleation sites or out of the reactor, further affecting the particle size. Prospects of this observed behaviour involve studying the kinetics of crystallization, which was beyond the scope of the present work. The size distribution was observed to vary less when 0.5 mL min−1 flow rate or higher was used, while at longer reaction time, i.e., slower flow rate, larger SD of the size of the particles was observed. After evaluating the STY, the conversion of TCPP, the size, and the size-distribution of the particles, the flow rate of 3 mL min−1 was selected as the best option. Slower flow rates were discarded due to lower STY, while higher flow rates did not show any enhancement of STY and instead resulted in less conversion of TCPP. As discussed in previous section, a flow rate of 3 mL min−1 implied a theoretical τ of 56 seconds. Since the flow profile of the reactor was defined as laminar with no secondary vortices, the variance of how much fluid passed through the reactor was calculated with the plug-flow residence time distribution function E(t) in eqn (7):40
![]() | (7) |
![]() | (8) |
It was observed that the mean residence time corresponded to 55 s, in good accordance with the theoretical τ. The variance (or square of the standard deviation), σ2, was calculated according to eqn (9):40
![]() | (9) |
The variance resulted 148.5 s2 (this moment indicates the spread of the distribution: the greater the value the greater the spread). Lastly, the skewness, s3, was calculated with eqn (10):40
![]() | (10) |
Skewness resulted 0.671 s3 (this moment measures the extent that a distribution is skewed in one direction or another in reference to the mean). Additional details of the curve of the concentration of the tracker, C(t), E(t) and the data to calculate the moments of RTD (tm, σ2, and s3) are reported in the ESI section-S7.†
:
Mod) was adjusted from 0.007 to 0.054 to explore the impact on particle size and STY. The results showed that particle size increased nearly linearly with the amount of acid used, while STY showed an inverse relationship, more marked, as illustrated in Fig. 4c. It is worth noting that inorganic and organic additives can be employed to control particle size by modifying crystallization. For instance, benzoic acid has been used as an additive to regulate particle size of different MOFs.38 Similarly, other acids such as HCl have been demonstrated to influence both nucleation and growth steps in the preparation of UiO-66.41 This suggests that the addition of different acids or other additives can be used to fine-tune the particle size and STY of the c.f. to achieve the desired properties for various applications. Based on the experimental results, it was found that TFA not only affected the crystal growth of PCN-222, but also the nucleation of the particles. It was also observed that the use of too much TFA led to the formation of larger particles and agglomerates with lower STY (see ESI section-S6† for additional details and SEM images). This is consistent with previous studies that have shown that the use of excessive amounts of acids can lead to the formation of large MOF particles and aggregates with poor crystallinity.42 Thus, to achieve a good balance between STY and particle size distribution, a L
:
Mod between 0.021 and 0.031 was found to be optimal. When operating with less acid (L
:
Mod 0.054), it was observed the formation of agglomerates of small particles (probably of ca. 30–40 nm). For subsequent experiments, a ligand-to-acid modulator ratio of 0.027 was thus chosen as it was found to provide a good compromise between particle size and STY with the minimum use of acid modulator.
The particle shape can significantly impact the behaviour of nanoparticles in various applications, including catalytic systems in continuous flow and drug delivery in the bloodstream. Research has indicated that prolate ellipsoids, with their elongated shape, exhibit unique hydrodynamic properties such as reduced drag and increased lateral migration in flow, enabling them to circulate for extended periods compared to spherical particles.17 This is particularly relevant in medical applications, where particles introduced into the bloodstream interact with blood components and encounter clearance mechanisms like the reticuloendothelial system, involving organs such as the liver and spleen. Controlling the spheroid aspect ratio of PCN-222 has not been reported to date, and achieving control during the synthesis step can be challenging. To address this, US was coupled with c.f. as an etching technique. Etching in the context of metal–organic frameworks (MOFs) refers to a process wherein the framework structure of a MOF is partially or completely removed using chemical or physical methods.
Various techniques, including the use of acids, bases, solvents, and external energy treatment, can achieve etching. However, the use of additional chemicals contradicts the principles of green chemistry (considering the increased amount of waste produced, or the potential use of toxic chemicals, etc.), making the treatment with external energy (e.g., heat transfer) a more sustainable option. Among these techniques, US-based etching represents a relatively recent and innovative approach for modifying MOF structures. As illustrated in Fig. 5, US was applied to the c.f. system (Reactor 2 in Fig. 2a) at amplitudes ranging from 20% to 90% (more than 90% amplitude is not recommended by the manufacturer) and its impact on particle morphology and STY was investigated (ESI section-S8†). The results revealed a linear increase in the aspect ratio of the particles with increasing US amplitude. While the mean particle length remained relatively constant, a higher SD of the size was observed. Additionally, as the US amplitude increased, the STY decreased, with the lower STY observed at 90% amplitude. These outcomes were attributed to localized pressure variations induced by US, leading to acoustic streaming and cavitation effects. Acoustic streaming, generated by the acoustic waves, involves a steady flow of fluid within the reactor. It facilitates fluid circulation, enhances mixing, and improves mass transfer and reaction kinetics. Cavitation occurs when the local pressure in the fluid drops below the vapor pressure, resulting in the formation and subsequent collapse of tiny vapor bubbles (at high local temperature). This phenomenon induces intense fluid motion, including microjets and shockwaves, which promote turbulence and enhance mixing. Two crucial observations were made. Firstly, the decrease in STY confirmed the etching of MOF crystals under the influence of US, as portions of the crystals were eroded, leading to diminished STY. Secondly, the increased SD in particle length increasing the US amplitude, indicate that the etching occurred at lower energy on the equatorial axis while at higher energy it occurred also on the polar axis (Fig. 5a). To confirm these observations, a complementary experiment was carried out by performing the US-etching with larger particles, highlighting superior changes in the aspect ratio, which increased from 2.72 ± 0.24 to 3.70 ± 0.33 (ESI Fig. S13†). The effect of the US-etching was further proven by a batch experiment redispersing, after purification, large particles of PCN-222 into fresh DMF, sequentially immersed in an US bath for 30 minutes. It was observed that the particles were etched by the US, resulting in particles with a higher aspect ratio (from 2.63 ± 0.15 to 4.22 ± 0.39, see ESI Fig. S14†). It should be noted that further investigation into US etching on PCN-222 would require computational simulations to fully investigate the breaking of the chemical bonds inside the MOFs in function of the applied US amplitude, which fall outside the scope of the present work.
N, N–H, C
C and C–H of the pyrrole ring in TCPP (Fig. 6b).43 The peak at 1676 cm−1 in TCPP was attributed to the stretching of the C
O bond, lowered in PCN-222 and indicating the coordination between –COOH and Zr atoms.43 The broad peak at ca. 3400 cm−1 corresponded to the stretching vibrations of N–H and O–H of the TCPP.44 TGA was employed to determine the phase transitions and decomposition temperatures of PCN-222 under air flow (Fig. 6c). The weight loss below 373 K was attributed to the removal of water/ethanol from the pores, followed by dehydroxylation of the Zr6 nodes between up to 723 K. The decomposition of TCPP ligands in the PCN-222 curve occurred beyond 693 K, leaving ZrO2 and carbon residues. The difference between the TGA profiles of PCN-222(0%US) and PCN-222(60%US) was determined by the same US, which generates more defect sites, resulting in a lighter material.18 PCN-222(0%US) and PCN-222(60%US) exhibited BET surface areas of 1801 m2 g−1 with pore volume of 1.69 cm3 g−1 and 1913 m2 g−1 with pore volume of 1.50 cm3 g−1, respectively. The BET surface areas were both based on the type IV N2-adsorption isotherm (Fig. 6d). The observed enhancement in the surface area parallel to the reduction in pore volume due to US treatment were consistent with the findings reported in the literature concerning the sonochemical synthesis of PCN-222.18
At the same time, it was observed that the use of DMSO led to higher inhomogeneity and in bigger particles. To obtain smaller particles and, more in general, to verify the control on the dimension of the particles, a study on the effect of the acid modulator was conducted (Fig. 7b). It was found that, comparted to the particles synthesized in DMF, a reduced amount of TFA was necessary to achieve a comparable small particle size, thereby increasing the green characteristics of the synthesis. For example, the E-factor and RME for the synthesis performed in DMF to obtain particles of 113 ± 27 nm (at 413 K and L
:
M = 0.027, refer to ESI Table S14†) were 46.6 and 2.1, respectively. When using DMSO as the solvent, the E-factor and RME to obtain PCN-222 of 116 ± 26 nm changed to 25.4 and 3.8%, respectively. However, in general, the quality of the particles, as indicated by a larger standard deviation in size (ESI Table S17†), was much lower than that of the particles produced using DMF. Additionally, the US-etching process was less efficient when using DMSO, resulting in no changes in the aspect ratio (2.38 ± 0.26 with 0% amplitude vs. 2.44 ± 0.37 with 60% amplitude), probably due to less affinity of DMSO in dissolving the etched crystals (thus not favouring the same etching). Consequently, the c.f. green synthesis of PCN-222 with DMSO may not be suitable for applications where a strict control of the morphology and of the dimension of the particles is crucial, such as for biomedical applications, where homogeneous particles with dimension less than 100 nm are needed,47 although more investigation must be carried out. However, the c.f. green synthesis of PCN-222 here discussed shows promise for progress in other fields, such as in catalysis and gas storage applications, where MOFs particles can be used also if showing relatively high inhomogeneity in terms of particle size.48,49
:
M = 1, L
:
Mod = 0.036, [TCPP] = 4.7 mM, flow rate 3 mL min−1, 60% US) with a DMF solution containing the S-GalNAc-PEG-sulfate ligand 8 in a concentration of 5 mg mL−1 (flow rate of the ligand solution: 3 mL min−1). This process yielded the PCN-222@SO3-PEG-S-GalNAc (Fig. 2c).11 The choice of a sulfate ligand was based on previous experiments, where a phosphate ligand was used on UiO-66.54 Compared to phosphate ligands, sulfate ligands were prepared using an innovative synthetic pathway that simplified the synthesis, provided better control, and yielded higher product quantities. Additionally, this approach eliminated lengthy purification steps such as three-day dialysis or the tedious separation of phosphate ligands from phosphoric acid. The successful loading of the ligand was confirmed through different analyses, as shown in Fig. 8.
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| Fig. 8 (a) FTIR analysis of PCN-222@ligand and (b) fluorescence microscopy images of the experiment of selective interaction of the PCN@SO3-PEG-S-GalNAc with lectins. | ||
FTIR spectroscopy (Fig. 8a) revealed the successful loading of the ligand on PCN-222 by the presence of characteristic peaks. Specifically, peaks observed at 2928 cm−1 and 2870 cm−1 were attributed to the asymmetric and symmetric stretching vibrations of the –CH2– group in the PEG chain,55 while peaks at 1245 cm−1 and 1135 cm−1 were attributed to the asymmetric and symmetric stretching vibrations of the sulfate (R–OSO3−) group.56,57 To further confirm the presence of the ligand bound to the MOF, a selective lectin interaction experiment was conducted (Fig. 8b, see ESI section-S11† for a scheme of the fluorescence microscopy experiment). Two variants of plant lectins were used and subsequently labelled for identification. One of them was Concanavalin A (ConA) of 26 kDa, obtained from the Canavalia ensiformis plant (jack bean), which was labelled with fluorescein isothiocyanate (FITC). The other lectin used was Peanut Agglutinin (PNA) of 110 kDa, obtained from peanuts (Arachis hypogaea), composed of four identical subunits of approximately 27 kDa each. PNA was labeled with AlexaFluor594 for identification. The sample preparation procedure is described in the ESI (section-S2†). Fluorescence was only detected in the case of the interaction with the PNA-AlexaFluor594 lectin (Fig. 8b), while it was not observed in the control experiment (PCN-222) and when ConA was used. This result confirmed the presence of thio-N-acetylgalactosamine, as the PNA lectin exhibits selective binding capability to this sugar. Additionally, the outcome suggested that PCN-222@SO3-PEG-S-GalNAc can establish specific interactions while being resistant to non-specific interactions, important for its use as drug delivery system. The literature also supports this observation, as it has been documented that Con A selectively binds to α-D-mannopyranosides, α-D-glucopyranosides, and, to a lesser extent, N-acetylglucosamines.57 On the other hand, the selectivity of the PNA lectin follows a preference trend for certain types of sugars: β-D-Gal-[1–3]-D-GalNAc > Gal > GalNAc.58 The presence of the ligand was also confirmed by TGA analysis (see ESI section-S11† for SEM images, XRD patterns and TGA profiles of PCN-222 vs. PCN-222@SO3-PEG-S-GalNAc).
The fluorescence microscopy images also unveiled the existence of agglomerates. This occurrence can be ascribed to the tetrameric nature of the PNA lectin, which enables the interconnection of various PCN-222@SO3-PEG-S-GalNAc entities, leading to the formation of agglomerates. SEM images of the PCN-222 and PCN-222@SO3-PEG-S-GalNAc showed no relevant differences (ESI section-S11†).
Footnote |
| † Electronic supplementary information (ESI) available: Details of the c.f. system; materials and methods; preliminary tests for batch optimization; relevant publications related to the c.f. synthesis of MOFs; calculation of Re, De and residence time (τ); details of the effect of the concentration of the reagents, the volumetric flow rate, the amount of employed acid modulator, and the temperature of the reactions on the STY and on the size-distribution of PCN-222; residence time distribution and pulse experiment; US-assisted techniques; DLS analysis of the samples PCN-222(0%US) and PCN-222(60%US); green approaches of the c.f. synthesis; functionalization with S-GalNAc-PEG-sulfate ligand and 1H-NMR and 13C-NMR spectra. See DOI: https://doi.org/10.1039/d3gc02774k |
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