Hannah F.
Mathews
ab,
Tolga
Çeper
cde,
Tobias
Speen
ab,
Céline
Bastard
ab,
Selin
Bulut
ab,
Maria I.
Pieper
ab,
Felix H.
Schacher
cdef,
Laura
De Laporte
abg and
Andrij
Pich
*abh
aDWI – Leibniz Institute for Interactive Materials, Forckenbeckstr. 50, 52074 Aachen, Germany. E-mail: pich@dwi.rwth-aachen.de
bInstitute of Technical and Macromolecular Chemistry, RWTH Aachen University, Worringer Weg 2, 52074 Aachen, Germany
cInstitute of Organic Chemistry and Macromolecular Chemistry, Friedrich-Schiller-University Jena, Humboldtstr. 10, 07743 Jena, Germany
dJena Center for Soft Matter (JCSM), Friedrich-Schiller-University Jena, Philosophenweg 7, 07743 Jena, Germany
eCenter for Energy and Environmental Chemistry Jena (CEEC), Friedrich-Schiller-University Jena, Philosophenweg 7a, 07743 Jena, Germany
fCluster of Excellence Balance of the Microverse, Friedrich-Schiller-University Jena, Grüne Aue, 07754 Jena, Germany
gInstitute of Applied Medical Engineering (AME), Department of Advanced Materials for Biomedicine (AMB), University Hospital RWTH Aachen, Center for Biohybrid Medical Systems (CMBS), Forckenbeckstr. 55, 52074 Aachen, Germany
hAachen Maastricht Institute for Biobased Materials (AMIBM), Brightland Chemelot Campus, Maastricht University, 6167 RD Geleen, The Netherlands
First published on 25th July 2024
Biomedical applications such as drug delivery, tissue engineering, and functional surface coating rely on switchable adsorption and desorption of specialized guest molecules. Poly(dehydroalanine), a polyzwitterion containing pH-dependent positive and negative charges, shows promise for such reversible loading, especially when integrated into a gel network. Herein, we present the fabrication of poly(dehydroalanine)-derived gels of different size scales and evaluate them with respect to their practical use in biomedicine. Already existing protocols for bulk gelation were remodeled to derive suitable reaction conditions for droplet-based microfluidic synthesis. Depending on the layout of the microfluidic chip, microgels with a size of approximately 30 μm or 200 μm were obtained, whose crosslinking density can be increased by implementing a multi-arm crosslinker. We analyzed the effects of the crosslinker species on composition, permeability, and softness and show that the microgels exhibit advantageous properties inherent to zwitterionic polymer systems, including high hydrophilicity as well as pH- and ionic strength-sensitivity. We demonstrate pH-regulated uptake and release of fluorescent model dyes before testing the adsorption of a small antimicrobial peptide, LL-37. Quantification of the peptide accommodated within the microgels reveals the impact of size and crosslinking density of the microgels. Biocompatibility of the microgels was validated by cell tests.
Polyzwitterions, i.e. polymers that carry both positively and negatively ionizable moieties within each monomer unit,11,12 have hence been extensively investigated. Due to their high charge density, they form strong intra- and intermolecular ion pairs, which result in charge compensation at intermediate pH values and an effective net charge of zero at the isoelectric point.13,14 The strong ion complexation within the polyzwitterions also limits their overall solubility, so that the use of polar protic solvents, the addition of salt, or the administration of heat is necessary to disrupt the attractive ionic interactions and solubilize the polymer.13,15,16 Because of the structural similarity between synthetic and natural polyzwitterions, it is often assumed that the synthetic polymers are biocompatible and exhibit resistance to biofouling17,18 even though corresponding studies have only been carried out for a few of the substances known from literature.16
Recently, the focus of research has shifted from synthetic polybetaines12,17,19 to polyzwitterions derived from natural building blocks. Li et al. introduced polyzwitterions adapted from trimethylamine N-oxide (TMAO), an osmolyte found in saltwater fish. The polymers (PTMAO) were prepared by oxidation of N,N-dimethylaminopropyl acrylamide followed by photopolymerization and exhibited antifouling properties as well as low immunogenicity.20 Feng and coworkers expanded on these findings and grafted PTMAO onto commercial polyamide filtration membranes by use of controlled atom transfer radical polymerization (ATRP). In this way, the membranes were endowed with enhanced fouling resistance whilst maintaining a comparatively low flux decline and sufficient water permeability.21
In addition to osmolytes, amino acids have been used as natural building block for polyzwitterions. Wang et al. used L-carnitine, formed through metabolism of methionine and lysine, and converted it with acryloyl chloride to the respective methacrylate, which they in turn grafted onto a gold surface by ATRP. Subsequent protein binding assays with fibrinogen and lysosome demonstrated that the proteins did not adsorb to the surface, and bacterial adhesion tests with E. coli confirmed an antifouling performance similar to that of polybetaines.22 Instead of L-carnitine, Leiske and coworkers modified glutamic acid to prepare zwitterionic monomers with different vinyl end groups. They then utilized reversible addition-fragmentation chain-transfer (RAFT) polymerization whilst protecting the carboxyl and amino groups to obtain defined polymers. The authors were particularly interested in the influence of the polymerizable group on the interaction of the polyzwitterions with cells, and proved that the association of the polymers with different cell types depends on the polymer backbone.23
Starting from the amino acid serine, the synthesis of the polyzwitterion poly(dehydroalanine) (PDha) is possible.24 In contrast to the common geometry of polybetaines, the oppositely charged groups in PDha are not located within the same pendant chain but in two separate side chains connected to the same backbone atom.12,24 The concurrent presence of both carboxylic acid and amine in every monomer unit provides PDha with pH-tunable characteristics: at low and high pH values, it behaves as polyelectrolyte with either polycationic or polyanionic traits, whereas it acts as polyzwitterion in the intermediate pH range.24,25 Though PDha was initially obtained by free radical polymerization of N-acetyl dehydroalanine followed by removal of the acetoxy group,26 it is nowadays mostly synthesized via the prepolymer species poly(tert-butoxycarbonylaminomethyl acrylate) (PtBAMA).24,27 Co-polymers of PDha have either been prepared by ATRP of tBAMA with polymeric halogenides and subsequent deprotection of the ionizable moieites27–30 or by post-modification of a fraction of the amino functions in the homopolymer.31–33
In the last years, the Schacher group has focussed on exploiting the co-existence of positive and negative charges within PDha for various applications. Magnetic nanoparticles (MNPs) coated with PDha34 were shown to adsorb and desorb polyelectrolyte model cargo by electrostatic interaction depending on the pH value of the surrounding medium.35,36 While the non-specific adsorption of proteins was less pronounced for PDha-treated nanoparticles than for pristine or polyanion-coated nanoparticles, they still displayed a protein corona.37 Çeper et al. produced organogels by crosslinking the prepolymer PtBAMA with N,N′-methylenebisacrylamide before hydrolysing the groups protecting the carboxylates and amines.38 Analogous to previous experiments with PDha-coated MNPs,35,36 pH-dependent uptake and release of anionic and cationic model dyes was verified.38 Hydrogel networks were synthesized by crosslinking PDha with bifunctional poly(ethylene glycol) diglycidylether (PEG-DGE).39,40 The ionic groups within the gel network allowed for the electrostatic adsorption of various catalytic species and charged photosensitizers enabling light-driven hydrogen and oxygen evolution reactions.39–41 In contrast to that, Kowalczuk et al. first synthesized asymmetric star-shaped block copolymers from PEG and PDha, which they later incorporated into PEG-based hydrogels via their terminal thiol functions using a photoinduced thiol–ene click reaction. In addition to the adsorption of model dyes, they demonstrated that the peptide sequence RGDS could be immobilized within the hydrogels. The authors interpreted this as an indication that PDha-based hydrogels have a high potential as scaffolds for tissue engineering.
Compared to traditional bulk hydrogels, microgels offer distinct advantages in the biomedical field.42–45 Especially polyzwitterionic microgels have been considered for drug delivery, tissue engineering and antibacterial or antifouling coatings.46,47 However, neither have corresponding materials from PDha been fabricated yet nor have the existing bulk hydrogel networks been tested concerning biocompatibility. Herein, we suggest a simple engineering approach, in which amine–epoxy crosslinking of PDha with PEG-epoxides31,39,40 is employed in droplet-based microfluidics to form microgels of adaptable size (Fig. 1). After microfluidic fabrication, we analyse the composition of the microgels and test the availability of residual amino groups by a fluorescamine assay. The behaviour of the microgels is evaluated and compared to the bulk hydrogel, especially concerning their potential in biomedical applications. In this regard, we examine permeability and determine the softness of the microgels by both nanoindentation and micropipette aspiration. By measuring the electrophoretic mobility and swelling degree of the microgels, we verify that the polyzwitterionic character of PDha endows the microgels with pH- and ionic strength-responsivity. Our experiments with model dyes and the antibacterial peptide LL-37 show that the electrostatic charges within the microgels also permit the accommodation of guest molecules within the network. Cell culture confirms that the microgels affect neither viability nor proliferation and are thus, biocompatible.
If not indicated otherwise, HPLC-grade water (VWR, filtered at 0.2 μm) was used for the experiments. Potassium hydroxide solution (KOH, ChemSolute, 0.1 M, ≥ 85.0%) was used as received. Formic acid buffers (pH 3.0–4.4), succinic acid buffers (pH 5.0–6.0), phosphoric acid buffers (pH 6.5–8.0), tris(hydroxymethyl)aminomethane (TRIS) buffers (pH 8.5–8.9), and N-cyclohexyl-3-aminopropanesulfonic acid (CAPS) buffers (pH 9.6–11.0) were prepared according to literature48 and adjusted to an ionic strength of I = 10 mM.
For the fabrication of the microfluidic chip, a polydimethylsiloxane (PDMS) silicone elastomer kit (SYLGARD 184, Downsil) was used. As oil phase in droplet-based microfluidics, a mixture of hydrofluoroether (HFE) oil and neutral surfactant (FluoSurf™ 2 w/w% in Novec7500, Emulseo) was employed.
Sulforhodamine B (sRB, Merck/Sigma Aldrich, 75%, 1 mg) and rhodamine 6G (R-6G, Merck/Sigma Aldrich, 1 mg) were solved in V = 1 mL of either formic acid buffer (pH 3.0, I = 10 mM), water (pH ≈ 6.5), or CAPS buffer (pH 11.0, I = 10 mM) to yield solutions of c = 1 mg mL−1. Fluorescein isothiocyanate-labelled dextrans (FITC-dextran, Merck/Sigma Aldrich) were employed without modification. Fluorescamine (Merck/Sigma Aldrich, ≥98%) was solved in acetone to obtain a solution with c = 3 mg mL−1. The fluorescein-conjugated cathelicidin antimicrobial peptide LL-37 (FITC-LL-37, Biozol/Rockland Immunochemicals, lyophilized, 1 mg) was solved in V = 1 mL water before its use in experiments.
Samplea | c(PDha) [mg mL−1] | Crosslinker | c(PEG-epoxide) [mg mL−1] | V(PDha)/V(PEG-epoxide) | m%theo(PDha) [wt%] |
---|---|---|---|---|---|
a HG indicates bulk hydrogel samples. Superscript signs indicate which PEG epoxy species was used (2: bifunctional PEG-DGE, 4: tetrafunctional 4arm-PEG-Ep, DA: bifunctional PEGDA). The brackets specify the theoretical weight percentage of PDha in the hydrogel. | |||||
HG2(13) | 25 | PEG-DGE (bifunctional) | 300 | 3:1 | ≈13 |
HG2(16) | 25 | PEG-DGE (bifunctional) | 400 | 3:1 | ≈16 |
HG2(20) | 25 | PEG-DGE (bifunctional) | 500 | 3:1 | ≈20 |
HG4(16) | 25 | 4arm-PEG-Ep (tetrafunctional) | 400 | 3:1 | ≈16 |
HGDA(16) | 25 | PEGDA (bifunctional) | 400 | 3:1 | ≈16 |
Samplea | Crosslinker | c(Crosslinker) [mg mL−1] | m%theo(PDha) [wt%] | m%1187(PDha)b [wt%] | m%1290(PDha)c [wt%] | No. of aqueous phases | h channel [μm] | D h [μm] |
---|---|---|---|---|---|---|---|---|
a MG indicates microgel samples fabricated with a microchannel height of 80 μm; mg indicates microgel samples fabricated with a microchannel height of 20 μm. Superscript signs indicate which PEG epoxy species was used (2: bifunctional PEG-DGE, 4: tetrafunctional 4arm-PEG-Ep). The brackets specify the theoretical weight percentage of PDha in the respective microgel. b Weight concentration of PDha within the respective microgel calculated by FT-IR spectroscopy exploiting the ratio between the C–N stretching vibration (1187 cm−1) of PDha and the C–O–C vibration (1100 cm−1) of the crosslink. c Weight concentration of PDha within the respective microgel calculated by FT-IR spectroscopy exploiting the ratio between the C–N valence vibration (1290 cm−1) of PDha and the C–O–C vibration (1100 cm−1) of the crosslink. d Hydrodynamic diameter of the respective microgel species as determined by optical microscopy in HPLC-grade water (average of 100 microgels measured). | ||||||||
MG2(13) | PEG-DGE | 500 | 13 | — | — | 1 | 80 | — |
MG2(16) | PEG-DGE | 400 | 16 | 28 | 30 | 1 | 80 | 297.4 ± 10.3 |
MG2(20) | PEG-DGE | 300 | 20 | 40 | 40 | 1 | 80 | — |
MG2(16)2w | PEG-DGE | 400 | 16 | 23 | 20 | 2 | 80 | 198.8 ± 63.4 |
mg2(16) | PEG-DGE | 400 | 16 | 34 | 34 | 1 | 20 | 35.9 ± 2.5 |
MG4(13) | 4arm-PEG-Ep | 500 | 13 | 17 | 30 | 1 | 80 | — |
MG4(16) | 4arm-PEG-Ep | 400 | 16 | 23 | 33 | 1 | 80 | 207.9 ± 7.8 |
MG4(20) | 4arm-PEG-Ep | 300 | 20 | 25 | 36 | 1 | 80 | — |
mg4(16) | 4arm-PEG-Ep | 400 | 16 | 37 | 23 | 1 | 20 | 28.5 ± 1.6 |
mg4(20) | 4arm-PEG-Ep | 300 | 20 | 34 | 30 | 1 | 20 | 33.2 ± 1.4 |
Purification of the formed microgels was achieved by successive solvent exchange. For that, the samples were allowed to sediment, the supernatant decanted and replaced with fresh solvent. In that way, the samples were washed thrice with HFE oil to remove the surfactant, twice with hexane to withdraw residual oil and at least five times with water to remove side products and unreacted polymer. As the microgels did not sediment as readily in water as they did in HFE oil and hexane, they were centrifuged (t = 30–60 s, 7500 rpm) prior to decantation and addition of fresh water.
Before using the microgel samples to load them with FITC-LL-37 peptide, they were centrifuged (t = 30–60 s, 7500 rpm) so the supernatant could be removed and a concentrated microgel sediment was obtained. The volume of the sediment (Vsediment) was necessary to approximate the number of microgels (Nmicrogel) per sample using the respective hydrodynamic diameter (Dh) as stated in (1).
(1) |
To each microgel sample, V = 50 μL of aqueous FITC-LL-37 solution (c = 1 mg mL−1) and V = 200 μL of water were added. The mixture was then left to shake in the dark for t = 1–2 d. Afterwards, the samples were filled with fresh water to V = 0.5 mL and purified by centrifugation (t = 1 min, 10000 rpm) before exchanging the supernatant. This procedure was repeated four times until the supernatant remained colourless and clear.
For the fluorometric assay of primary amine groups, V = 200 μL of the respective microgel dispersion were placed onto an object slide and thoroughly mixed with V = 10 μL of a fluorescamine solution (c = 3 mg mL−1 in acetone). Microscopic analysis was performed using a diode 405 UV laser (3% intensity, λexc = 405 nm) with a HyD detector (gain: 300%, λem = 455–500 nm, pinhole: 1.00) for fluorescence and a PMT trans detector for brightfield images.
The uptake of fluorescent dyes was investigated by applying V = 20 μL of the respective microgel sample onto an object slide and recording fluorescence and brightfield images. The fluorophore sRB was excited with a diode pumped solid state (DPSS) laser (3–4% intensity, λexc = 561 nm) and the resulting fluorescence detected with a HyD detector (gain: 400%, λem = 575–620 nm, pinhole: 1.00), while the fluorophore R-6G was excited with the argon laser (10%, 1% intensity, λexc = 514 nm) and its fluorescence detected with a HyD detector (gain: 50%, λem = 530–570 nm, pinhole: 1.00). Brightfield images were taken with the PMT trans detector in both cases.
The diffusion of FITC-dextrans of varying molecular weight into the microgels was assessed by redispersing V = 50 μL of concentrated microgel sediment in the respective FITC-dextran solutions (c = 1 mg mL−1; Mw = 4 kDa, 40 kDa and 150 kDa). The samples were investigated with an argon laser (10%, 1% intensity, λexc = 488 nm) combined with a HyD detector (λem = 500–550 nm, pinhole: 1.00) and PMT trans detector. For the permeability studies, the gain was adjusted so that the fluorescence intensity of the surrounding medium was approximately 100 RFU for all samples.
The adsorption of FITC-labelled LL-37 peptide into the microgels was verified using analogous instrument settings and a HyD gain of 10–40%.
To determine the effective Young's modulus (E-modulus, E), homogeneity of the sample was assumed and a simple continuum-medium model (2) used.52 The force F exerted on the microgel was calculated from the applied pressure Δp and the pipette radius (RP = 32.5 μm) according to eqn (3) before plotting it against the normalized aspirated length Δx of the microgel. The term ϕP, which exhibits a partial dependency on the thickness of the pipette wall, is customarily assumed to be ϕP = 2.1. Consequently, the effective Young's modulus was calculated using the slope s of the linear fit (4).
Δp/E = (2πΔx)/(3ϕPRP) | (2) |
F = Δp·π·RP2 | (3) |
E = s(3ϕP)/(2π2RP) | (4) |
The respective PDha-based microgel samples were washed twice with DMEM containing 10% FCS and 1% ABM. Subsequently, the microgel dispersions were diluted to c ≈ 300 microgels per μL for the small microgels (mg) or c ≈ 20 microgels per μL for the large microgels (MG). Prior to their use in cell experiments, all microgel dispersions were sterilized by UV irradiation (t = 30 min).
First, we tested the bulk gelation under reaction conditions suitable for use in PDMS-based droplet-based microfluidics. Due to the poor solubility of PDha (Fig. S2, ESI†),24,25 the reaction was carried out in aqueous KOH (0.1 M, pH 13). As Çeper et al. had found the bulk hydrogels to be self-supporting only when PEG-DGE with Mn = 2000 Da was used and claimed that gelation proceeded best with Pi(PDha) = 180,40 we directly employed the corresponding reactive polymers. In addition to the sample with PEG-DGE (HG2(16)), we also conducted bulk gelation trials with PEGDA (HGDA(16)) and 4arm-PEG-Ep (HG4(16)), the former to open up an alternative reaction route via aza-Michael addition, the latter to create a more finely meshed gel. To facilitate the realization of the reaction in droplet-based microfluidics, the gelation had to proceed at room temperature (rt). In contrast to previous research,39,40 gelation therefore took t = 2 d before the inverted vial test indicated successful gel formation (Fig. 1(b)). While the sample HGDA(16) did not yield a stable gel and was thus discarded for follow-up experiments, both samples containing epoxide-based PEG crosslinker formed pliable transparent bulk hydrogels.
Rheological analysis was performed for PEG-DGE crosslinked bulk hydrogels with varying amounts of crosslinker and a 4arm-PEG-Ep crosslinked bulk hydrogel (Table 1) 2 d after initial mixing. In all samples, the elastic modulus (G′) is larger than the viscous modulus (G′′) in the linear viscoelastic region (LVR) (Fig. S3(a), ESI†). Outside of the LVR, the hydrogels display a distinct G′′ maximum. The breakdown of the gel is hence characterized by the rupture of an increasing number of individual bonds (micro cracks) until a macro crack forms, which results in viscous flow of the sample. In HG2 samples, the crossover point shifts to larger strains with decreasing amounts of PEG-DGE, which suggests that not the crosslinker but PDha is reliable for the mitigation of the micro cracks. Possibly, the amine and carboxylic acid functions form dynamic intra- and intermolecular hydrogen bonds, limiting the movement of the broken chains.40
In time sweeps, a constant and parallel progression of the G′ and G′′ plots with G′ > G′′ implies that the hydrogels are fully cured and in kinetic equilibrium (Fig. S3(b), ESI†). Frequency sweeps show that G′ exceeds G′′ even towards low frequencies (Fig. S3(c), ESI†). As tan(δ) < 0.1 for all samples, the elastic, more solid-like characteristics of the hydrogels predominate. Interestingly, G′ of our PEG-DGE crosslinked bulk hydrogels is significantly lower compared to G′ of previously synthesized PDha-based hydrogels.39,40 The lower reaction temperature (rt vs. T = 60 °C) and thus, longer reaction time probably lead to increased hydrolysis of the terminal epoxy groups of the crosslinker and thus, to a lower yield of the crosslinking reaction.54 Increasing the crosslinker content in PEG-DGE crosslinked hydrogels did not necessarily lead to a higher elastic modulus. The reason for this may be that the amine groups in PDha contribute significantly to elasticity through hydrogen bonding and that PEG microdomains impair overall stability. Repeated application of high strain (outside of LVR) followed by relaxation at low strain (within the LVR) demonstrated complete regeneration in HG2(16) (Fig. S3(d), ESI†). Therefore, it is likely that the mechanical properties of the hydrogel are dominated by non-covalent dynamic interactions, such as electrostatic interaction and hydrogen bonding. This hypothesis could be verified in the future by varying the degree of crosslinking: if non-covalent interactions are indeed decisive, the behaviour of the hydrogels should remain mostly unaffected.
Carrying out post-polymerization crosslinking reactions in emulsified droplets has generally been shown to generate microgels.55–58 However, batch emulsion polymerization techniques often suffer from a broad size distribution of the microgels produced, which in turn renders characterization difficult. Therefore, we opted for a lithographic droplet-based microfluidic approach. Fluorinated oil mixed with the neutral surfactant FluoSurf™ was used as continuous phase, as it does not introduce additional charges to the system and ensures long-term stability of the product emulsion. As rheological analysis of the bulk hydrogels showed that the network strength did not improve significantly below m%(PDha) = 16 wt%, we focussed on the compositions with m%(PDha) ≥ 16 wt% and adopted the reaction conditions of the bulk hydrogel synthesis in the microfluidic approach as well. Analogously, the product emulsions were left to gel for 2 d after microfluidic droplet generation before they were purified by solvent exchange (Fig. 1(c) and (d)). The ratio between the flow rate of the oil and the flow rate of the aqueous phase(s) was set to 2:1 to avoid jetting of the dispersed phase and still achieve a sufficient flow of the more viscous water phase(s). To fabricate microgels of varying size, two different microfluidic devices with a channel height of 20 μm and 80 μm, respectively, were employed (Fig. S5, ESI†). Droplet formation occurred at the crossflow junction, where the shear force between oil and water phase prompted the generation of dispersed aqueous droplets (Fig. 1(c)).
The use of two separate water phases (one with the PEG-based crosslinker, one with the reactive polymer PDha) proved disadvantageous because the viscous aqueous solutions did not mix well within the channel. This resulted in a low PDha content and thus, structural instability of the microgels (Table 2 and Fig. S6, ESI†). Instead, the aqueous solutions were mixed prior to their transfer into the respective syringe and employed as a singular dispersed phase, since the gelation process took several hours (Fig. S4, ESI†).
Stable microgels were obtained that had a spherical morphology and appeared almost transparent in aqueous solution. Compared to the original height of the channel, the microgels had a significantly larger hydrodynamic diameter Dh, though this effect was more pronounced in the larger MG2(16) and MG4(16) samples than in the microgels prepared within the 20 μm channel. Since the aqueous droplets inside the microfluidic channel are elongated and become round only when exiting the microfluidic device, a comparatively larger hydrodynamic diameter of the microgels is to be expected. The size of the PDha-based microgels, however, corresponds to ≥150% of the initial height of the channel. On the one hand, the large hydrodynamic diameter can be attributed to the strong water affinity of PDha and thus, the high degree of swelling of the gel networks.40 On the other hand, a larger initial size of the microgels seems to further the swelling, presumably, because the pores within the MG2(16) and MG4(16) networks are larger and hence, promote the diffusion of water. Microgels containing lesser amounts of PEG-based crosslinker, e.g. mg4(20) (Table 2), are larger in size compared to microgels including more crosslinker, e.g. mg4(16) (Table 2). A higher fraction of terminal epoxy groups results in more crosslinking sites, so that the entire network becomes more tightly meshed and can therefore no longer swell as much as a less crosslinked system. The microgels with a lower overall crosslinker content are, however, structurally less stable than the more highly crosslinked samples, and suffer more strongly from droplet coalescence during the 2-day resting phase. The implementation of tetrafunctional 4arm-PEG-Ep as opposed to bifunctional PEG-DGE also leads to a denser, more crosslinked network which in turn results in smaller microgels with a narrower size distribution (Table 2 and Fig. S7, ESI†).
After purification and lyophilisation, the composition of the microgels was examined by FT-IR spectroscopy (Fig. 2). The successful integration of the PEG-based crosslinker is clearly confirmed by the signal of the C–O–C vibration (1100 cm−1) and additionally verified by the C–H valence vibration (2870 cm−1).39,59 The sharp epoxy signal at 1059 cm−1, clearly visible in both PEG-DGE and 4arm-PEG-Ep reference, disappears in the gel samples.60 While the acidic functions of PDha are clearly visible due to their CO vibration at 1685 cm−1, the amine groups are hidden as shoulder signals at 1600 cm−1 (N–H deformation), 1555 cm−1 (R–NH3+ deformation), and 1290 cm−1 (C–N valence vibration).39,59 Only the weak signal at 1187 cm−1 attributed to C–N stretching motions manifests as a stand-alone peak.61 By comparing the C–O–C signal (1100 cm−1) with the C–N valence signal (1290 cm−1) and the C–N stretching signal (1187 cm−1), respectively, a rough estimation of the weight fraction of PDha incorporated in the microgels was provided (Table 2 and Fig. S8, ESI†). Similar to the observations made for PDha-based hydrogels,40 the experimentally determined amount of PDha within the microgels is significantly higher than the theoretical value (Table 2). This may be explained by the fact that some of the epoxy groups of the respective PEG-based crosslinker are hydrolysed and therefore do not participate in the crosslinking reaction. Instead, the polymer strands are removed during purification, at least if they are not retained in the microgels due to chain entanglements.
In addition to FT-IR spectroscopy, we performed a proof-of-principle fluorometric assay to verify the presence of residual primary amine groups in the microgels. The organic spiro compound fluorescamine reacts with primary amine moieties to form a fluorescent diaryl-2-hydroxypyrrolinone derivative.62,63 Since fluorescamine only emits fluorescence after derivatization, a fluorescent signal within microgel samples after addition of fluorescamine can be considered as evidence of primary amine functions. Fig. 2 demonstrates that mg2(16), mg4(16), MG2(16), and MG4(16) all display fluorescence in the CLSM overlay images (λem = 455–500 nm). Decreased intensity in mg4(16) indicates a lower concentration of the fluorophore within the respective microgel. A possible reason for this might be that the smaller size of the initial droplet and the multiple arms of the crosslinker lead to a higher conversion of the amine–epoxy reaction, resulting in lower numbers of primary amine functions. However, smaller pores within the gel network may also limit the diffusion of fluorescamine, either because of the high hydrophilicity within the microgel network or as a consequence of spatial limitations.
For the larger microgel samples MG2(16) and MG4(16), we were able to evaluate the spatial limitations within the microgels by exploiting the correlation between different molecular weights of FITC-dextran and their corresponding hydrodynamic radius as published by Ambati et al.64 After equilibration of the respective microgel sample in an aqueous FITC-dextran solution of either 4 kDa, 40 kDa, or 150 kDa, the mixtures were subjected to CLSM. Relating the fluorescence intensity outside the microgels to the intensity within the microgels allows for an assessment regarding the ability of the respective FITC-dextran to permeate the network. Our results show that only FITC-dextran with M = 4 kDa (estimated Rh = 1.3 nm64) partially diffuses into the microgels whereas FITC-dextrans of higher molecular weights barely penetrate the microgels (Fig. S10, ESI†). While ca. 40% of 4 kDa FITC-dextran diffuse into MG2(16), the permeability is decreased for MG4(16), with only 26% of 4 kDa FITC-dextran passing into the network. This substantiates our claim that the multiple arms of the crosslinker lead to a more densely crosslinked system. Given that the mesh size of the microgels dictates their diffusivity, the permeability of FITC-dextran is poorer in MG4(16) than in MG2(16). On the basis of these experiments, it is, however, not possible to determine the exact pore size of the microgels, since electrostatic and hydrophobic interactions also influence diffusivity.
Regarding a potential biomedical use case, the mechanical properties of the microgels are decisive for their applicability. In tissue engineering, stem cell lineage specification may be governed by the softness of the surrounding matrix.65 When considering a use in tissue engineering or in vivo, the characteristics of the target organ are often mimicked by the malleability of the gel network.66,67 Therefore, we exemplarily investigated the mechanical properties of the microgel samples MG2(16) and MG4(16) by nanoindentation and MPA. Smaller microgel samples could, unfortunately, not be evaluated by these methods as the small size caused the cantilever tip to slide off the microgels in nanoindentation and made it difficult to visualize the microgel–water interface during MPA experiments. The microscopic images of the aspirated MG2(16) and MG4(16) microgels as well as the resulting linear fits are summarized in Fig. S9 (ESI†).
Fig. 3 graphically shows the effective Young's modulus of the respective microgels as measured by nanoindentation and MPA analysis. As was already discovered for the bulk hydrogels in rheology, the microgels appear to be very soft with E < 10 kPa, which is comparative to the E-modulus of muscle tissue.65 Generally, a high softness correlates with large mesh sizes, which is at odds with the previous observations concerning permeability. A potential explanation for this phenomenon may be that crosslinking within the microgels is only partially based on covalent bonds. Intra-colloidal electrostatic attraction and synergistic hydrogen bonds might allow the microgels to adapt dynamically to mechanical stress, thus rationalizing the observed softness. Both in nanoindentation and MPA experiments, MG4(16) demonstrates a higher E-modulus than MG2(16). MPA analysis provided slightly larger moduli, most likely due to adhesive forces between the capillary wall and the microgels tested. Overall, the results from nanoindentation and MPA measurements are in good agreement.
Fig. 3 Effective Young's modulus E as determined for large microgels MG2(16) and MG4(16) by MPA and nanoindentation. All microgels are relatively soft, comparative to the E-modulus of muscle tissue. |
Possibly the most interesting feature of the PDha-based microgels is their ability to switch their overall net charge depending on the surrounding pH-value. We therefore studied the response of the microgels to changes in pH value and ionic strength (Fig. 4). For pH-dependent measurements, the microgels were redispersed in buffer solutions with a fixed ionic strength of I = 10 mM to keep the effects caused by the salt concentration as low as possible whilst maintaining a constant pH value. As MG2(16) was expected to exhibit the most prominent charge alteration, we examined the respective microgels by electrophoretic light scattering even though in these measurements a measurement error caused by the gravity-induced sedimentation of the microgels must be taken into account. Still, the results in Fig. 4(a) demonstrate that the surface charge of the microgels is slightly positive in acidic environment (pH 3) and becomes gradually more negative with increasing pH value. At pH 3, i.e. around the pKA value of the carboxylic acid functions,68 both acidic and basic moieties are protonated so that the microgels are predominantly positively charged. Above the pKA value of the carboxylic acid, the respective functions get deprotonated, resulting in a negative charge that compensates the positive charges from the R–NH3+ groups. As a certain percentage of the amino moieties are sacrificed to fabricate the network, the ratio between amino and carboxyl groups is not equimolar but shifted in favour of the carboxyl functions. Thus, the isoelectric point in the microgels is also shifted towards lower pH values when compared to the reactive polymer PDha.24 At higher pH values, the amino groups start to deprotonate so that the overall charge decreases even further.
Following our verification of positive and negative charges within the microgel, we studied the swelling behaviour of the samples depending on the pH value (Fig. 4(b) and Fig. S11, ESI†). All samples show an initial increase in size up to a pH value of approximately pH 7 before the hydrodynamic diameter plateaus. Usually, this curve progression is typical for polyelectrolyte microgels with weakly acidic functions.69,70 As the ratio between amino and carboxyl groups is not equimolar, we hypothesize that the influence of the protonated, i.e. positively charged amino groups is compensated for by charge- and partial-charge dependent interactions. Similar considerations have already been disclosed in the context of the published bulk hydrogels from PDha.40 Compared to their size at pH 3, the size of the microgels fabricated with 4arm-PEG-Ep crosslinker only increased by approximately 10%, whereas the microgels containing PEG-DGE grew larger (Fig. 4(b) and Fig. S11, ESI†). Although this observation is valid for both the larger (MG) and the smaller microgels (mg), the trend is more apparent in the MG samples (Fig. 4(b)), as the comparatively large standard deviation in mg2(16) and mg4(16) makes the interpretation of the data more difficult (Fig. S11(c), ESI†). This observation is congruent with the fact that the tighter the crosslinking is, the lesser the ability of the gel to swell. As evident in Fig. 4(b), a decrease in crosslinker in the PEG-DGE-crosslinked microgels leads to a more pronounced swelling (35% increase in MG2(20) vis-à-vis 22% increase in MG2(16) and 12% increase in MG2(13)) but for samples crosslinked with 4arm-PEG-Ep, the amount of crosslinker does not lead to a significant change in swelling ratio. This suggests that maximum crosslinking is already achieved in the sample MG4(20) (and potentially, MG2(13)). Most likely, the degree of crosslinking is limited by the mobility of the PEG-based crosslinker within the network, which is more strongly impaired for the multi-arm compound than for the bifunctional molecule.
Since the microgels prepared with intermediate amounts of PEG-based crosslinker (mgx(16) and MGx(16)) proved the most robust against mechanical forces exerted during centrifugation while simultaneously exhibiting responsivity indicative of the respective microgel series, they were selected as representative samples for all following experiments. To evaluate the effect of ionic strength on the size of the PDha-based microgels, we redispersed the microgels in aqueous sodium chloride solutions of varying NaCl concentration. With an increase in ionic strength, the hydrodynamic diameter of the microgels decreased (Fig. 4(c) and Fig. S11(d), ESI†). In contrast to the pH-responsive swelling, this ionic strength-induced decrease in size is independent of the crosslinker species used. The reduction of size with rising salt concentration is usually typical for weak polyelectrolyte microgels in their charged state: here, the addition of salt leads to the screening of like-charges that induce electrostatic repulsion and thus, swelling. Consequently, the swelling degree of polyelectrolyte networks decreases with an increase in screening ions.71–73 Based on our electrophoretic mobility measurements of the surface charge (Fig. 4(a)) and the pH value of HPLC-grade water (≈6.5), we assume that in pure water, the PDha-based microgels are predominantly negatively charged. Internal salt bridges with carboxylic acid functions and hydrogen bond formation may compensate for the influence of the basic amino groups. Thus, the addition of salt results in a decrease in electrostatic repulsion by screening the carboxylate functions, which in turn leads to deswelling of the microgels.
The polyzwitterionic character of PDha and the polyampholyte properties of the gel network allow for the pH-regulated uptake and release of charged (bio-) molecules. Corresponding findings have already been reported with other, chemically different PDha-based bulk hydrogel systems by demonstrating the ad- and desorption of positively charged methylene blue and negatively charged methyl blue or acid orange 7, respectively.30,38 For our studies on PDha-based microgels, we decided to perform similar experiments with fluorescent dyes instead, since the visualization of conventional dyes is challenging due to the low concentration of dye within individual microgels. As model for positively charged compounds, we used rhodamine 6G (R-6G), and as model for negatively charged compounds, sulforhodamine B (sRB). These fluorescent dyes were selected because their fluorescence was shown to be independent of the pH value in a range from pH 3 to pH 10, and because both R-6G and sRB are highly water-soluble.74,75 The fluorescent dyes were dissolved in either formic acid buffer (pH 3), water or CAPS buffer (pH 11) and mixed with microgels to enable electrostatically-driven uptake. Subsequently, excess dye was removed by allowing the microgels to sediment and replacing the supernatant several times with the respective fresh solvent.
The samples were then subjected to CLSM to verify pH-dependent adsorption. Fig. 5 exemplarily shows the resulting images for MG2(16) and a scheme of the assumed underlying mechanism. In formic acid buffer, i.e. pH 3, MG2(16) is slightly positively charged (Fig. 4(a)) due to the protonation of the amino moieties. Thus, negatively charged sRB is adsorbed into the microgels and not retrieved even by extensive washing, whereas positively charged R-6G is completely removed from the sample by solvent exchange (Fig. 5, left). In water, MG2(16) presumably has a polyampholyte character, with carboxylate groups outweighing the positive charges. Under these conditions, a significant uptake of R-6G can be observed, whereas hardly any sRB remains in the network (Fig. 5, middle). The remaining amount of sRB could either stem from interaction with individual amino groups, which remain available due to the low ionic strength of the environment, or could be caused by other interactions, such as dipole–dipole or hydrophobic interactions. In CAPS buffer, i.e. pH 11, the adsorption of sRB into the microgels is minimal (Fig. 5, lower right). Experiments with R-6G in highly basic environments remained inconclusive as the R-6G dye formed aggregates and could not be removed from the supernatant even after numerous washing cycles (Fig. 5, upper right).
Addition of formic acid buffer (pH 3) to MG2(16) loaded with R-6G in water induced a significant decrease in fluorescence intensity, whereas only a slight decrease in fluorescence intensity could be observed, when MG2(16), previously loaded with sRB under acidic conditions, was treated with basic CAPS buffer (pH 11) (Fig. S12, ESI†). The desorption of cationic R-6G was fuelled by a change both in pH value and ionic strength: the acidic pH value of the buffer was below the pKA of the carboxylic acid, thus inducing protonation of the carboxylate groups, while the higher salt concentration (Ibuffer > Iwater) caused charge screening and osmotic pressure effects. In contrast, the addition of CAPS buffer to the formerly acidic microgel dispersion containing sRB did not change ionic strength, and the resultant pH value was only raised to intermediate values as formic acid and basic buffer were mixed. Nevertheless, the reduction of fluorescence intensity also suggests a release of the model dye in this sample.
To give a more specific example of the biomedical potential of the microgels, their loading with a bioactive substance was tested. We decided to examine targeted peptide transport with the PDha-based microgels as the concept is studied not only in the context of therapy but also in surface modification.76–78 As model substance, FITC-labelled LL-37 (FITC-LL-37), a human antimicrobial peptide derived from the cathelicidin hCAP-18,79 was selected. LL-37 comprises 37 amino acids, with multiple lysine and arginine residues contributing to the overall cationic charge of the peptide. While it adopts a random coil conformation in water, it occurs as α-helix in specific salt solutions.80 We decided to use already labelled LL-37 for our experiments to easily visualize the uptake by CLSM. As with the model dyes, microgel samples and peptide were mixed to enable uptake by electrostatic attraction before excess FITC-LL-37 was separated by decanting and replacing the supernatant.
Subsequently, the fluorescence intensity was measured both in the samples and in the total collected supernatant solution. A fluorescence calibration curve determined for FITC-LL-37 (Fig. S13, ESI†) then allowed for the deduction of the respective concentration of FITC-LL-37 in the microgels and in the corresponding supernatant. Comparison of the resulting total concentration with the amount of peptide originally implemented showed reasonable consistency of the values (Fig. 6(a)). By approximating a perfectly spherical morphology of the microgels, we specified their volume and thus, could calculate the number of microgels per sample using their respective average hydrodynamic diameter (1). This allowed for the deduction that mg2(16) adsorbed approximately 1.0 pg FITC-LL-37 per microgel, whereas mg4(16) took up about 0.5 pg (Fig. 6(b)). For the larger microgels, the loading was increased (Fig. 6(c)) to 166.0 pg for MG2(16) and 102.9 pg for MG4(16). The difference in uptake between the smaller (mg) and the larger (MG) samples corresponds roughly to their volume ratio. As was to be expected from the permeability assay (Fig. S9, ESI†), the microgels containing bifunctional PEG-DGE crosslinker adsorb substantially higher amounts of FITC-LL-37 than the microgels containing tetrafunctional 4arm-PEG-Ep. Interestingly, the amount of peptide accommodated is about one and a half to two times higher in mg2(16)/MG2(16) than in mg4(16)/MG4(16). This matches the observation in the pH-responsive swelling, where the PEG-DGE crosslinked samples mg2(16)/MG2(16) demonstrate a swelling of 20% whereas 4arm-PEG-Ep crosslinked samples mg4(16)/MG4(16) exhibit an increase in size of only 10%. Follow-up experiments are intended to fine-tune the crosslinking within the microgels and optimize uptake. Additionally, future research should determine whether the LL-37 integrated into the gels presents in its active, α-helix conformation (as it has in previous studies)77 or remains in a random coil.
A biomedical application of the presented PDha-based gel networks is only feasible if the samples are highly biocompatible. Previous cell tests conducted with linear PDha or PDha-coated nanoparticles and human brain microvascular endothelial cells showed no apparent short-term cytotoxicity.34,37 We assessed biocompatibility by cultivating the respective microgel samples with normal human dermal fibroblasts (NHDFs) for t = 24 h and t = 7 d, respectively, before performing a live/dead assay to monitor cell viability (Fig. 7). Although the microgels took up the dead reagent (BOBO™-3 iodide), likely due to electrostatic attraction to the carboxylate groups, the fluorescence images do not show a substantial effect on cell viability induced by the microgels. Extending the duration of the experiment (t = 7 d) led to similar results as t = 1 d of culture (Fig. 7(a) and (b)). Fluorescence-based evaluation of cell proliferation indicated that cell growth in the samples with microgels progressed identically to the positive control (Fig. 7(c)). Our in vitro experiments suggest that the PDha-based microgels are fully biotolerant and non-cytotoxic.
As of yet, the microgels presented in this study are too large for drug delivery systems, particularly in human medicine. However, as shown, the microfluidic approach allows for facile optimization of the morphology and size, so that oral administration of drug-loaded microgels is conceivable in the future. The discovery that the E-modulus of the PDha-based microgels is in the myogenic range may also prove interesting for potential muscle tissue engineering approaches. The established electrostatic and dynamic interactions could be exploited to form switchable microporous annealed particle hydrogels, which have been found advantageous for cell spreading and proliferation.81
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4sm00676c |
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