Sebastian
Bonardd‡
ab,
Binoy
Maiti‡
c,
Santiago
Grijalvo
d,
Jacqueline
Rodríguez
ab,
Hamidreza
Enshaei
e,
Galder
Kortaberria
f,
Carlos
Alemán
eg and
David
Díaz Díaz
*abh
aDepartmento de Química Orgánica, Universidad de La Laguna, Avda. Astrofísico Francisco Sánchez 3, La Laguna 38206, Tenerife, Spain. E-mail: ddiazdiaz@ull.edu.es
bInstituto Universitario de Bio-Orgánica Antonio González, Universidad de La Laguna, Avda. Astrofísico Francisco Sánchez 2, La Laguna 38206, Tenerife, Spain
cSchool of Chemistry & Biochemistry, Georgia Institute of Technology, 901 Atlantic Dr NW, Atlanta, GA 30332, USA
dNetworking Center on Bioengineering, Biomaterials and Nanomedicine (CIBER-BBN), Jordi Girona 18-26, 08034 Barcelona, Spain
eDepartament d’Enginyeria Química and Barcelona Research Center in Multiscale Science and Engineering, IMEM-BRT, EEBE, Universitat Politècnica de Catalunya, C/Eduard Maristany, 10-14, Ed. I, 08019, Barcelona, Spain
fMaterials + Technologies” Group, Chemical & Environmental Engineering Department, Basque Country University, Plaza Europa 1, 20018, Donostia, Spain
gInstitute for Bioengineering of Catalonia (IBEC), The Barcelona Institute of Science and Technology, Baldiri Reixac 10-12, 08028, Barcelona, Spain
hInstitute of Organic Chemistry, University of Regensburg, Universitätstr. 31, Regensburg 93053, Germany
First published on 16th June 2022
Herein, we describe the design and synthesis of a new variety of bio-based hydrogel films using a Cu(I)-catalyzed photo-click reaction. These films exhibited thermal-triggered swelling–deswelling and were constructed by crosslinking a triazide derivative of glycerol ethoxylate and dialkyne structures derived from isosorbide, a well-known plant-based platform molecule. The success of the click reaction was corroborated through infrared spectroscopy (FTIR) and the smooth surface of the obtained films was confirmed by scanning electron microscopy (SEM). The thermal characterization was carried out in terms of thermogravimetry (TGA) and differential scanning calorimetry (DSC), from which the decomposition onset and glass transition temperatures were determined, respectively. Additionally, mechanical properties of the samples were estimated by stress–strain experiments. Then, their swelling and deswelling properties were systematically examined in PBS buffer, revealing a thermoresponsive behavior that was successfully tested in the release of the anticancer drug doxorubicin. We also confirmed the non-cytotoxicity of these materials, which is a fundamental aspect for their potential use as drug carriers or tissue engineering matrices.
Within this context, hydrogels are a special class of polymeric networks, which can absorb and retain a large amount of water while preserving their three-dimensional integrity. Due to their high water content, many hydrogels are biocompatible and show similar properties to natural tissue, which makes them suitable for biomedical applications.4–8 In recent years, increasing attention have been paid to stimuli-responsive hydrogels that can sense and respond to external stimuli, such as temperature, pH, light, electrical fields, etc.9–12 In particular, thermoresponsive hydrogels are one class of the most widely studied stimuli-responsive hydrogels with great potential for drug delivery systems.13–16
Recently, we have reported the synthesis of a new series of hydrogels composed of glycerol ethoxylate and bisphenol A-based monomers.17 The water-swollen hydrogel membranes displayed thermoresponsive actuation and lower critical solution temperature (LCST). In this work, motivated by the potential of these materials as drug delivery systems, and considering the potential toxicity of bisphenol A-derivatives, we decided to redesign the formulation using glycerol ethoxylate and biomass-derived isosorbide monomers.
The above mesityl derivative (4.00 g, 3.00 mmol) was dissolved in 50 mL of dry N,N-dimethylformamide (DMF), after which sodium azide (0.98 g, 15.00 mmol) was added in one single portion allowing the reaction to proceed under constant stirring at 70 °C overnight. After this time, the mixture was noted to be a fine white suspension that was filtered affording a clear, homogeneous yellow-brown supernatant. DMF was removed under reduce pressure and the resultant crude oil triturated with 100 mL of ethyl acetate. The mixture was then sonicated for 15 min and filtered using 30 mL medium fritted glass funnel. The achieved brown filtrate was washed twice with 100 mL of distilled water and once with 100 mL of brine. The organic phase was dried overnight using Na2SO4 and concentrated to afford the triazide derivative in 70% yield. Spectroscopic data were in good agreement with those reported in the literature.181H NMR (CDCl3): δ 3.64–3.54 (m, –CH2–CH2–O–), 3.33 (t, –CH2–N3).
NOTE: Although we have not experience any safety problem handling triazide 1a, it should be emphasized that small organic azides can be heat- and shock-sensitive. As a general recommendation, they should never be distilled to dryness or stored in the absence of solvent.
(1) |
Once the maximum swollen state was established, the deswelling process of these samples was evaluated in terms of the water retention parameter (WR, eqn (2)). The initially swollen sample of weight Wo, equilibrated at 22 °C, was rapidly transferred to a PBS buffer solution at 37 °C or 50 °C aiming to evaluate this process at two different temperatures. Then, similar to the above protocol, after different time intervals the film was withdrawn from the hot solution, gently dried with tissue paper and weighted to record Wt values.
(2) |
(3) |
For release experiments, the above preswollen drug-loaded membranes were rinsed with PBS buffer prior to be introduced into glass vials containing 10 mL of PBS buffer solutions preheated at 37 °C and 50 °C. Immediately after membrane immersion, the absorbance of the supernatant was measured at different time intervals by extracting 1 mL of the receptor phase, while the total volume of the experiment was maintained by adding 1 mL of fresh PBS solution. Cumulative drug release profiles were used to evaluate the evolution of the process.
Additionally, three kinetic models were selected to fit to the cumulative DOX released as a function of time: (i) Peppas–Sahlin equation (eqn (4)); (ii) Weibull model (eqn (5)); and (iii) Korsmeyer–Peppas (eqn (6)). Mt and M∞ are the cumulative and maximum of drug released at time “t”. In eqn (4), K1 is a constant that corresponds to the release rate of the diffusion process whereas K2 corresponds to the polymer relaxation.20 In Weibull equation model, K is a constant and b corresponds to the diffusion mechanism. A Fickian mechanism is described when b ≤ 0.75. Other processes involving complex release mechanisms are described when 0.75 < b < 1.21 Finally, KH is a constant value and n is the diffusional exponent, in the case of eqn 6.22 An Excel plugin namely DDSolver23 was used to evaluate the DOX release data and be interpreted with various kinetic models in order to estimate the appropriate release mechanism of DOX from the composite material.
(4) |
(5) |
(6) |
Qualitatively, the success of this protocol was initially confirmed after obtaining a transparent and bendable solid film from both liquid precursors (Fig. 1A). A direct comparison between FTIR spectra recorded for 1a, 1b and the film can be conducted from Fig. 1B. The spectrum of the triazide precursor revealed an intense band centered at 2106 cm−1 demonstrating the presence of the azide group, while the presence of the terminal alkyne functionality in the isosorbide derivate was confirmed by the detection of a broad and high intensity band positioned around 3270 cm−1 (C–H vibration) as well as a low intensity signal centered at 2115 cm−1 (CC vibration mode). Moreover, as was expected, the FTIR spectra of both precursors allow the detection of aliphatic C–H vibrations appearing in the range between 3000–2800 cm−1 where, in the case of 1b, two separated signals can be observed. This could be attributed to the cyclic structure of this precursor, which has been previously reported for other aliphatic cycles.24 Furthermore, the presence of C–O–C linkages in both molecules was demonstrated through the presence of a strong and broad signal centered around 1120 and 1080 cm−1. Using the above information, the FTIR analysis of films confirmed the success of the photo-click reaction due to the complete absence of signals ascribed to azides and alkynes functionalities, while bands related to the presence of C–H and C–O–C structures remained in the spectrum. In addition, a small group of signals (pointed by a black arrow in Fig. 1B) appeared between 1600–1500 cm−1 that could be assigned to the presence of triazole structures.25–27 Finally, Fig. 1C exhibits a SEM image showing a smooth and homogeneous surface morphology, along with a rougher edge that could be caused by the cutting process used to prepare the sample.
Fig. 1 (A) Digital images of obtained flexible hydrogel films (diameter of circular film = 4 cm). (B) FTIR spectra of 1a, 1b and the film. (C) SEM image of the hydrogel film. Scale bar = 300 μm. |
After confirming the success of the light-triggered crosslinking process, the obtained films were subjected to stress–strain measurements in order to evaluate their mechanical properties (Fig. S1, ESI†). From the above results, values of 5.75 ± 1.55 MPa, 114.03 ± 27.22 MPa and 1.90 ± 0.12 MPa were calculated for stress at break, elongation at break and Young's modulus parameters, respectively. In previous works,17 we have successfully carried out the reticulation of glycerol ethoxylate derivatives using diverse bifunctional molecules, such as bisphenol A diazide and 4,4′-methylenebis(cyclohexyl isocyanate), among others.17 Thus, taking the aforementioned materials as reference, the values of the mechanical properties obtained in this work are within the same range as those obtained previously.17 However, a deeper comparison between the obtained material and its previously published counterparts shows higher values of Young's modulus and stress at break, along with a lower elongation at break for the former. These parameters have been previously associated with the nature of the hard segments in these crosslinked materials,17 which in this case would correspond to the isosorbide structure. Unlike the previously used molecules,17 isosorbide is characterized by its lower size and its more strained structure. Thereby, the reticulation process of glycerol ethoxylate units by isosorbide-based structures seems to induce the formation of polymer films exhibiting greater mechanical strength but lower elongation capacity. Notwithstanding the above, with an elongation at break value above 100%, the as-prepared film can be considered as a material with an adequate elasticity. Furthermore, thermal properties of synthesized membrane was investigated by TGA and DSC (Fig. 2).
Fig. 2 (A) TGA and DTGA profiles obtained for a dry film. (B) DSC curves measured for a water-swollen sample. |
TGA analysis reveals two weight loss steps, being the first one (centered at ca. 100 °C) assigned to the volatilization of adsorbed moisture and remaining water retained within the film coming from the washing process. In contrast, the second step would be ascribed to the degradation of the material itself. This decomposition is represented in the DTGA profile as a peak centered at 384 °C (labeled as TMD), temperature at which the maximum degradation rate is reached. However, a more detailed analysis of the peak revealed that, at higher temperatures, its symmetry is broken accusing the presence of a third process merged with this degradation step. Considering the chemical structure of the material, abundant in ether bonds coming from both precursors, a feasible degradation mechanism could be interpreted as the random fragmentation of the polymer network through this type of linkages, giving way to the volatilization of low molecular weight species. In addition to the above, the merged process identified at higher temperatures could originate after the cleavage of more thermally stable chemical structures, such as remains of isosorbide-based entities and/or triazole units responsible for the crosslinking sites in the polymer matrix. Finally, the onset degradation temperature (Tonset), referred as the temperature at which the material loses 5% of its initial weight, occurs at 355 °C. Thus, this material meets most of the thermal requirements to be considered in a wide spectrum of applications, including biomedical ones. On the other hand, since DSC was carried out between temperatures where no degradation phenomena take place, we decided to conduct the experiment starting from a 24 h water-swollen film to study its thermal behavior in the presence and absence of water, aiming to start focusing the present study towards the analysis of these films in hydrogel state. It is well-known that PEG-based materials exhibit a LCST behavior which, in some cases, can be detected as an endothermic process during DSC measurements.17,28–30 Above this temperature, hydrogen bonds between water molecules and polymer chains are disrupted, generating the dehydration of the material along with a phase separation that is usually evidenced by the appearance of turbidity in the sample. For pure PEG systems, the LCST behavior is achieved near to boiling conditions,31,32 whereas by adjusting the amphiphilic nature of the system, for example, by adding hydrophobic structures into the polymer backbone, the LCST temperature can be notably decreased.33,34 In previous works, by means of DSC, our group has been able to detect LCST temperatures in different glycerol ethoxylate membranes cross-linked with molecules of marked hydrophobic character.17 Some of these membranes also acquired an opalescent appearance when heated above this temperature. Unfortunately, contrary to the above, in this case we were not capable of detect a clear LCST behavior instead, an intense and asymmetric endothermic peak centered at 87.6 °C was visualized during the heating process of the swollen film (Fig. 2B). This transition would be mostly related to the evaporation of water; however, it should be noted that the observed asymmetry is generated by a subtle increase of the recorded signal starting from temperatures far enough from volatilization processes (≈ 35 °C, the dotted line in Fig. 2B is just for orientational purposes), therefore, we cannot discard the occurrence of other phenomena (e.g. water evaporation) that are eclipsed by the main signal at lower temperatures. We will complement this discussion later, during the evaluation of the swelling–deswelling properties of the material. Finally, after completing the first heating process, now the dry sample was subjected to two consecutive cooling and heating steps, in which a completely amorphous behavior was observed in the whole temperature range, detecting a glass transition temperature (Tg) centered at −27.1 °C (pointed by black arrows in Fig. 2B). After completing the structural, mechanical and thermal characterization of films, the properties of these materials as swellable hydrogels for drug delivery applications were evaluated (Fig. 3).
The first test conducted was the evaluation of the swelling kinetics during the immersion of a dried piece of material into PBS buffer at 22 °C. Fig. 3A exhibits the evolution of the swelling ratio (eqn (1)) through time showing that after 60 min of immersion a plateau is reached. This plateau is characterized by a maximum swelling ratio of 366%, being more than 3 times higher than the one previously reported for glycerol ethoxylate membranes reticulated with bisphenol entities.17 The hydrophobic character of the isosorbide-based monomer is lower than that of the bisphenol-based monomer. Therefore, by using isosorbide structures as crosslinking agents, the well-known hydrophilic property of glycerol ethoxylate would be less affected, being traduced not only in a higher swelling ratio but also in a faster swelling process. Then, the deswelling process of a fully PBS-swollen hydrogel film was evaluated at two temperatures, 37 °C and 50 °C, separately. Surprisingly, at both temperatures the hydrogel showed deswelling, being more pronounced at the higher temperature. The deswelling kinetics was achieved by measuring the evolution through time of the water retention parameter (eqn (2)), which results are shown in Fig. 3B. It can be seen that at both temperatures this parameter drops rapidly at the beginning of the process, and then gradually decreases as the hydrogel reaches a certain dehydrated state. More importantly, at higher temperatures, lower values are achieved, and the process takes place more rapidly. The calculated water retention values from the plateau regions were 77% and 69% at 37 °C and 50 °C, respectively. The value recorded at 50 °C is notably higher than the one previously reported for the system reticulated with bisphenol units, meaning that the deswelling process in this material is less pronounced. Again, this could be ascribed to the more hydrophilic character of the system which would require higher temperatures to favor the hydrogel dehydration. Although this system managed to exhibit a thermoresponsive behavior attributed to its swelling–deswelling ability, the markedly less favored deswelling process along with the absence of a clear LCST behavior could be related to the poor hydrophilic–hydrophobic balance achieved in the material. Nevertheless, we show that once the plateau value is reached, the water retention value can continue to decrease by transferring the sample to a warmer medium (Fig. S2, ESI†). Finally, the stability against the pH of these hydrogels was assessed by immersing them for prolongated times into different aqueous buffer solutions. Results displayed in Fig. 3C demonstrate that these materials, regardless the pH value, did not reveal quantifiable mass losses even after 96 h of incubation. Therefore, since no traces of material should be released to the surrounding media, we decided to attempt the evaluation of the biocompatible properties of our system in cell culture using the MTT assay35 (Fig. 3D). Thus, high and low concentrations of the film (6.07, 3.03, and 0.76 mg mL−1) were selected to study the effect induced by the material on cellular proliferation. To do so, HeLa cells were used as a model cell line and were incubated in the presence of appropriate material concentrations for 24 h at 37 °C. As shown in Fig. 3D, the three tested concentrations showed similar behavior if compared with non-treated cells with cellular viabilities over 90% suggesting that the material is non-cytotoxic. These results might confirm the potential use of our material for biomedical applications, supporting the idea of using isosorbide structures as crosslinking agents in PEG-based materials.
Finally, motivated by the thermoresponsive behavior showed by these hydrogels, along with their adequate biocompatibility, we test our material as a temperature-controlled delivery system using anticancer drug doxorubicin (Fig. 4).
The loading of the drug within hydrogel films was conducted by immersing a dry piece of sample into an aqueous PBS buffer solution of DOX·HCl. The process was followed by recording the absorbance of the supernatant at different time intervals as is shown in Fig. 4A. Moreover, aiming to a more quantitative analysis, the adsorption efficiency parameter (eqn (3)) was calculated and evaluated as function of time (Fig. 4B). The adsorption profile reveals that the material was able to remove from the solution 80% of the drug during the first 5 h of the experiment, approaching to a plateau state after 10 h. Based on the above, the dye adsorption efficiency after 24 h was 92%. During the process, the solution was gradually decolored while the hydrated film adopted an intense red color. It should be noted that, while the equilibrium swelling is reached at 60 min, the drug adsorption process continues for at least 10 more hours. Therefore, based on our results, it is plausible to infer that most of the drug adsorption takes place once the material reaches its maximum state of hydration. In this sense, the adsorption process would be mostly commanded by non-covalent interactions taking place between the drug and the hydrogel structure rather than water uptake. Then, the in vitro drug release of DOX-loaded hydrogels was evaluated in PBS buffer solution at 37 °C and 50 °C for 24 h (Fig. 4C). Interestingly, the encapsulated DOX displayed an initial burst release at early stage (17% and 25% in the first 30 min for incubations at 37 °C and 50 °C, respectively). The release profiles followed a controlled behavior in both cases reaching a plateau value within a period of 24 h. Specifically, the amount of DOX released was about 38% at 37 °C and 40% at 50 °C, respectively. As expected from deswelling measurements, release profiles obtained at 50 °C showed faster release kinetics along with slightly higher drug release. Thus, decreasing the temperature of the experiment from 50 to 37 °C enabled to increase the release time period from 150 to 300 min at which the maximum amount of drug is released.
Three models were used to describe the DOX release kinetics from the hydrogel film: (i) Peppas–Sahlin, (ii) Weibull distribution, and (iii) Korsmeyer–Peppas. These models have been extensively selected to give insight into the release mechanism of drugs from polymeric drug delivery systems making distinction between Fickian or non-Fickian diffusions. The release kinetic parameters are displayed in Table S1 (ESI†). The best correlation coefficient (R2) was obtained from the Weibull distribution (0.98) if compared with the Peppas–Sahlin (0.97) and Korsmeyer–Peppas (0.89) equations by plotting % cumulative DOX release against time (min). Taking the Weibull model as the most consistent one, we noticed the diffusion exponent was less than 0.75 (b = 0.56) indicating a Fickian diffusion mechanism of DOX (Fig. S3, ESI†). However, this model is empirical and faces some deficiencies36 so the comparison with other semi-empirical release models is common. In this sense, we selected the Peppas–Sahlin model to describe the release behavior of DOX. This model showed a diffusional exponent m of 0.45 which confirmed the Fickian diffusion mechanism during the incubation process as described with Weibull.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2sm00623e |
‡ These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2022 |