Open Access Article
Haobo Hong†
a,
Tshepiso L. Tema†ab,
Redoy Gazi Shuvoa,
Harald Rupp
c,
Stephanie Krügerd,
Anja Marinow
*a,
Zviadi Katcharava
*ab and
Wolfgang H. Binder
*ab
aMacromolecular Chemistry, Division of Technical and Macromolecular Chemistry, Faculty of Natural Sciences II (Chemistry, Physics, Mathematics), Institute of Chemistry, Martin Luther University Halle-Wittenberg, von-Danckelmann-Platz 4, D-06120 Halle, Germany. E-mail: anja.marinow@chemie.uni-halle.de; zviadi.katcharava@chemie.uni-halle.de
bDesign of 3D-Printable Polymers Based on Regional Resources, Just Transition Center, Martin-Luther-University of Halle-Wittenberg University, 06099 Halle, Germany
cInstitut für Kunststofftechnologie und -recycling e.V., 06369 Weißandt-Gölzau, Germany
dBiocenter, Microscopy Unit, Martin Luther University Halle-Wittenberg, Weinbergweg 22, 06120 Halle/Saale, Germany
First published on 13th May 2026
Flame-retardant and reprocessable gel composites composed of a pyrrolidinium-based poly(ionic liquid) were successfully prepared by incorporating surface-modified SiO2-nanoparticles functionalized with ionic liquids or multiple hydrogen bonding groups (ureidopyrimidinones). Covalent functionalization was verified by CP-MAS 29Si NMR, FT-IR, and thermogravimetric analysis. Surface-modified NPs significantly improved the dynamic characteristics of the synthesized gel composites, yielding composites with enhanced reprocessability and remarkable mechanical flexibility, reaching an elongation at break of up to 460%, achieved solely through reversible dynamic interactions without the need for permanent covalent crosslinking. Upon reprocessing, the ionic conductivity of the gels was efficiently restored, reaching values of 2.2 × 10−4 S cm−1 at room temperature. The composites further exhibited excellent thermal stability up to 330 °C and an inherently flame-retardant nature classified as UL 94 V-0 grade. These combined features underscore the potential of the developed PIL-based gel composites for safe, durable, and high-performance applications in electrochemical and flexible devices.
In this study, we report the development of flame-retardant, stretchable, reprocessable, and conductive materials based on dynamic poly(ionic liquid) network composites. Gel polymer electrolytes require reprocessability not only from the perspective of sustainability, but also to enhance the lifetime and economic features of advanced battery systems. In addition, during battery manufacturing, processing defects such as incomplete wetting, film imperfections, or inhomogeneous thickness may occur. Reprocessable gel electrolytes therefore allow the correction of defects without complete disposal of the material, thereby significantly improving manufacturing efficiency. Our design strategy here is centered around silica nanoparticles whose surfaces were modified with two different functional groups to impart compatibility with the surrounding matrix and allow for dynamic properties inside the electrolyte. Firstly, ureidopyrimidinone (UPy), which forms strong and reversible quadruple hydrogen bonds, was embedded to create dynamic crosslinks and enhance mechanical properties;25–27 secondly we used modified ionic liquid moieties to improve nanoparticle dispersibility and promote ionic interactions throughout the polymer network.24,28–30
Our approach focuses on formulating PIL gels and composites that combine safety, flexibility, and high ionic conductivity. Pyrrolidinium-based ionic liquids and the corresponding monomers were chosen due to their outstanding electrochemical and thermal stability.31 The influence of silica nanofillers with different surface chemistries on the structural and electrochemical behavior of the gels was systematically explored. A schematic overview of the designed gel structure is shown in Fig. 1, illustrating the main components: a pyrrolidinium-based acrylate monomer that polymerizes to form the PIL backbone; a UPy monomer, integrated into the polymer network to introduce reversible supramolecular interactions that enhance reprocessability and mechanical resilience; a mobile ionic phase, consisting of a pyrrolidinium-based ionic liquid (PMPyrr TFSI) and lithium salt (LiTFSI), providing the primary ionic conduction pathway; surface-modified silica nanofillers, acting as a reinforcing agent promoting dynamic crosslinking and high stretchability; and a photoinitiator to enable UV-curing during material fabrication.
This work aims to establish a versatile design concept for multicomponent PIL-based composite gels that unite safety, flexibility, and high ionic mobility.
Cross-polarization (CP) magic-angle spinning (MAS) solid-state NMR spectra of 29Si were recorded at ambient temperature on a Bruker Avance II 400 spectrometer, equipped with a 4 mm MAS probe, with an MAS of 5 kHz, a CP time of 10 ms and a repetition delay of 5 s.
Thermogravimetric analysis (TGA) was conducted on a Netzsch TG 209 F3. Samples (5–15 mg) were placed in alumina crucibles and heated from 35 °C to 800 °C at a heating rate of 10 K min−1 under a nitrogen atmosphere (flow rate: 20 mL min−1). The NETZSCH Proteus was used for analyzing the recorded data.
Fourier-transform infrared spectroscopy (FT-IR) analysis was conducted using the attenuated total reflection technique on a VERTEX 70v FT-IR spectrometer (Bruker) equipped with the Golden Gate diamond ATR unit. Measurements were conducted at room temperature in the spectral range of 550–4000 cm−1.
Dynamic light scattering (DLS) analysis was performed using a Litesizer 500 (Anton Paar) equipped with a 40 mW single-frequency laser diode (at a wavelength of 658 nm). All data were processed using Kalliope software.
Tensile tests were conducted using an INSTRON 5900 Series universal testing system machine. Dumbbell samples (ISO 37 Type 2) were produced using a pneumatic cutter (P-VS 3000, MonTech Rubber Testing Solutions). Measurements were performed at room temperature at a strain rate of 20 mm min−1. Data analysis was performed via Bluehill Universal (version 4.08).
Broadband dielectric spectroscopy (BDS) was used for investigating ionic conductivities on a Novocontrol “Alpha analyzer”. PIL gels were placed between two brass electrodes (d = 20 mm), and the thickness of each sample gel was measured individually (sample thickness ranged from 0.20 mm to 0.50 mm). The measuring cell was placed in a cryostat with a constant flow of dry nitrogen. Ionic conductivity was recorded in the frequency range of 1–106 Hz and at different temperatures. Ion conductivity values were extracted from the plateau of σ vs. T.
Reprocessing of gel composites was done using a vacuum compression molding (VCM) tool from MeltPrep. The sample was placed in the VCM disc tool with a diameter of 20 mm and heated at 120 °C for 3 hours. Subsequently, the tool was placed in the cooling unit and the restored sample was removed.
In the second step, 1 g of NP-NH2 (1 g) was dispersed in dry CHCl3 (100 mL), and subsequently, 1-(6-isocyanatohexyl)-3-(4-methyl-6-oxo-1,6-dihydropyrimidin-2-yl)urea (UPy-NCO) (0.62 g, 2.1 mmol, previously synthesized according to the literature34) was added. The reaction was refluxed under an inert atmosphere for 24 h. The modified particles were washed with CHCl3 for removing unreacted (6-isocyanatohexyl)-3-(4-methyl-6-oxo-1,6-dihydropyrimidin-2-yl)urea. NP-UPy was collected by centrifugation and dried in an oven at 60 °C under vacuum (1.2 g of product obtained).
NP-IL was prepared by a previously described procedure.29 Initially, N-[3-(trimethoxy silyl)propyl]-N-methylpyrrolidinium chloride was prepared with the following procedure: a mixture of N-methylpyrrolidinium (5 mL, 47 mmol) and (3-chloropropyl)trimethoxysilane (8.57 mL, 47 mmol) was kept at 80 °C while stirring for 48 hours under an inert atmosphere. The red/orangish mixture was washed using diethyl ether (4 times), and the obtained product was dried in a vacuum. The yield was 45%. 1H NMR (CDCl3, 400 MHz, δ in ppm): 3.78–3.61 (m, 4H), 3.54–3.47 (m, 2H), 3.45 (s, 9H), 3.19 (s, 3H), 2.27–2.08 (m, 4H), 1.80–1.68 (m, 2H), 0.61–0.53 (m, 2H). 13C NMR (CDCl3, 101 MHz, δ in ppm): 65.36, 64.15, 50.62, 48.40, 21.5, 17.59, 5.77.
A Ludox-sm® silica nanoparticle solution (3 g) was diluted with deionized water (100 g), and 0.7 g (2.5 mmol) of N-[3-(trimethoxysilyl)propyl]-N-methylpyrrolidinium chloride was added to the solution. The mixture was stirred continuously at 80 °C for 24 hours. Modified nanoparticles were concentrated using a rotary evaporator and precipitated into acetone. NP-Cl was collected using centrifugation and washed with acetone three more times. Subsequently, NP-CL (4.5 g) was dissolved in 120 mL of deionized water and mixed with 20 mL of a solution containing 4 g (14 mmol) LiTFSI. The mixture was kept for stirring for 8 hours at room temperature, after which the final product was collected via centrifugation and washed with deionized water (4 times). NP-IL was dried under vacuum at 70 °C for 24 hours.
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| Fig. 2 (A) Chemical structure of surface-modified NPs, (B) Si29 CP MAS solid-state NMR, (C) FT-IR spectra of surface modified nanoparticles, (D) thermogravimetric analysis, (E) size distribution of surface-modified NPs and (F) corresponding TEM images. | ||
Additionally, the decrease in the Q3 peak intensity (around −100 ppm) after modification indicates a reduction in the number of silanol groups, which is consistent with successful covalent functionalization of the silica nanoparticles. Fig. 2C shows the IR spectra of the nanoparticles, highlighting the appearance of alkyl C–H stretching vibrations (2800–3000 cm−1) after surface modification. NP-IL exhibits characteristic bands of the TFSI− counterion at 1349 cm−1 (SO2 stretching) and 1179 cm−1 (CF3 stretching).38,39 On the other hand, NP-UPy shows new bands in the 1400–1700 cm−1 region, corresponding to C
O, C–N, and N–H bond vibrations, confirming successful functionalization.40–42 Thermogravimetric analysis was employed to quantify the degree of surface modification (Fig. 2D), assuming that the observed weight loss primarily arises from the degradation of the organic surface layer, while contributions from moisture evaporation and dihydroxylation are negligible. The TGA thermograms (Fig. 2D) display the mass loss of Ludox-sm®, NP-NH2, NP-UPy, and NP-IL. Based on these values, the concentration of ionic liquid functional groups in NP-IL was calculated to be 0.81 mmol g−1, while NP-UPy exhibited functional group concentrations of 0.68 mmol g−1. Ludox SM is reported to have a specific surface area of 320–400 m2 g−1. According to the literature, the surface silanol density can be approximated as 5 OH per nm2,43 thereby estimating the total number of hydroxyl groups of Ludox SM to be (1.6–2.0) × 1021 OH per gram, corresponding to 2.66–3.32 mmol g−1. Since we cannot exactly assess the fractions of the bi-(T2) or tri-(T3) siloxane linkages, the precise extent of the surface modification is difficult to determine. Assuming that attachment sites with T3 predominate, the estimated extent of surface modification is 85–91% for NP-IL and 61–77% for NP-UPy.
The size of the nanoparticles was monitored throughout the modification process to ensure that the particles remained within the expected range. The starting material (Ludox® SM) with an average particle diameter of 7 nm exhibited a gradual increase in size after each functionalization step. NP-NH2 showed the smallest average diameter, followed by NP-IL and NP-UPy. Dynamic light scattering (Fig. 2E) analysis indicated that NP-UPy exhibited a hydrodynamic diameter exceeding 100 nm, which is attributed to supramolecular aggregation driven by the strong UPy–UPy interactions. This clustering behavior was further verified by transmission electron microscopy (Fig. 2F), which showed the presence of aggregated domains. In contrast, NP-IL exhibited a smaller hydrodynamic radius, consistent with the TEM observations of well-dispersed particles and reduced aggregation (for comparison see also ESI, Fig. S9 and S10).
In our previous investigation, formulations devoid of NPs included 1,6-hexanediol dimethacrylate as a covalent crosslinker.32 Covalent crosslinker effectively enhanced the gel's stretchability, but it simultaneously reduced its ability to self-heal or be reprocessed due to the formation of permanent networks. In the present work, we eliminated the 1,6-hexanediol dimethacrylate crosslinker to promote dynamic and reversible interactions, compensating for the potential loss in mechanical strength by incorporating surface-modified nanofillers.
Our approach focused on introducing nanofillers while maintaining the other components constant, to understand the effect of nanoparticle incorporation prior to further optimization. The prepared compositions are summarized in Table 1. G1 serves as the reference sample, containing the covalent crosslinker but no nanofillers. Formulations incorporating 5 and 10 wt% of NP-IL (G2 and G3, respectively) exhibited a reduction in ionic conductivity from 1.1 × 10−4 S cm−1 (G1) to 9.5 × 10−5 S cm−1 (G2) and 6.9 × 10−5 S cm−1 (G3) at room temperature. Although NP-IL possesses abundant ionic liquid moieties on its surface, its presence likely restricts the mobility of the polymer chains and decreases the overall ionic conductivity. A similar trend was observed in mechanical testing (Fig. 4A): the reference gel G1 showed the highest elongation at break, whereas G2 and G3 fractured at lower elongations. Subsequently, we prepared gel formulations without covalent crosslinkers but with additional nanofillers (keeping the molar ratio of M-IL and M-UPy constant). A comparison between G2 (containing a covalent crosslinker) and its counterpart G4 (without the covalent crosslinker) revealed a significant improvement in mechanical flexibility. Elongation at break increased from 146% (G2) to 466% (G4) – a more than threefold enhancement (Fig. 4B). Additionally, the tensile strength rose from 0.58 MPa to 0.83 MPa, indicating that the nanofillers contributed to reinforcement of the polymer network. Further increasing the NP-IL content slightly reduced the elongation at break to 386% (G6), suggesting that excessive filler loading may lead to reduced chain mobility.
| Sample | Covalent crosslinker | Molar ratios | IL (wt%) | Li salt (wt%) | Nanofiller | Nanofiller amount (wt%) | Conductivity at RT (S cm−1) | Tensile strength (MPa) | Elongation at break (%) | ||
|---|---|---|---|---|---|---|---|---|---|---|---|
| M-IL | M-UPy | C | |||||||||
| G1 | + | 10.4 | 8 | 1 | 48.7 | 16.3 | — | — | 1.1 × 10−4 | 0.66 | 189 |
| G2 | + | 10.4 | 8 | 1 | 46.3 | 15.4 | NP-IL | 5 | 9.5 × 10−5 | 0.58 | 145 |
| G3 | + | 10.4 | 8 | 1 | 43.5 | 14.6 | NP-IL | 10 | 6.9 × 10−5 | 0.73 | 146 |
| G4 | − | 10.4 | 8 | 0 | 46.3 | 15.4 | NP-IL | 5 | 2.2 × 10−4 | 0.83 | 466 |
| G5 | − | 10.4 | 8 | 0 | 43.5 | 14.6 | NP-IL | 10 | 1.2 × 10−4 | 0.86 | 437 |
| G6 | − | 10.4 | 8 | 0 | 41.4 | 13.8 | NP-IL | 15 | 8.7 × 10−5 | 0.9 | 386 |
| G7 | − | 10.4 | 8 | 0 | 46.3 | 15.4 | NP-UPy | 1 | 1.3 × 10−4 | 0.87 | 483 |
| G8 | − | 10.4 | 8 | 0 | 43.5 | 14.6 | NP-UPy | 5 | 1.8 × 10−4 | 0.85 | 424 |
A similar behavior was observed for composites containing NP-UPy (Fig. 4C). However, the incorporation of NP-UPy was limited to below 5 wt% as higher contents led to reduced dispersivity, forming non-transparent samples. This is presumably due to strong interparticle interactions, which promote aggregation. In contrast, NP-IL could be incorporated at higher concentrations as a result of improved dispersibility by IL-functionalized surfaces (better chemical compatibility with the ionic liquid-based polymer matrix). The ionic conductivity of the gel composites was characterized using broadband dielectric spectroscopy (BDS) over a temperature range of −20 to 70 °C (see ESI, Fig. S11–S18). In a typical measurement, the dielectric response was recorded across a frequency range of 10–107 Hz. The resulting frequency-dependent conductivity curves (Fig. 4D) exhibit a distinct plateau region at each temperature, from which the DC conductivity values were extracted. A significant increase in conductivity was observed with increasing temperatures, as expected. The temperature-dependent conductivity plots for the gel composites (Fig. 4E) display a nonlinear relationship, characteristic of polymer-based electrolytes. This behavior follows the Vogel–Tammann–Fulcher (VTF) model (ESI, Fig. S3),44,45 which describes ion transport in polymeric systems and reflects the dynamic nature of the gel matrices. Among the studied samples, G4 exhibited the highest conductivity values across the entire temperature range. With the incorporation of only 5 wt% NP-IL, G4 achieved a maximum conductivity of 2.7 mS cm−1 at 70 °C. A comparison between G4 and G2 indicates that the removal of the covalent crosslinker and the addition of NP-ILs resulted in a more than two-fold improvement in conductivity across all temperatures (Fig. 4F). Furthermore, the ionic conductivity of the gel composites was evaluated after 12 months of storage in a glovebox and showed no significant change compared to the pristine material, confirming the good long-term stability of the prepared gel composites (ESI, Fig. S23).
In addition to ionic conductivity, the thermal and safety properties of the polymer electrolytes were evaluated. Thermogravimetric analysis (Fig. 5A) confirmed that the composites exhibited excellent thermal stability, with no significant weight loss up to 330 °C for NP-IL-containing formulations. In contrast, systems utilizing NP-UPy particles showed degradation onset above 250 °C, indicating a lower thermal stability limit for those materials. Another critical parameter for electrolyte safety is flammability. As shown in Fig. 5B, the gel composites are entirely flame retardant. In a simple test, a direct flame was applied to the specimen for 10 seconds. The material neither ignited nor exhibited any visible degradation. These observations were further confirmed by UL 94 flammability tests, in which the material achieved a V-0 grading for a thickness of 1 mm (see ESI, Table S1 and Fig. S22), demonstrating its excellent flame retardancy and suitability for safe electrochemical applications.
The introduction of additional dynamic interactions (ionic interactions derived from NP-IL and supramolecular hydrogen-bonding interactions contributed by NP-UPy) was expected to enhance the reprocessability of the gel composites. To evaluate this, broken gel fragments were placed into a mold and reprocessed using a hot-vacuum press at 120 °C for 3 hours. The results of this procedure are presented in Fig. 6A. Regardless of the type or amount of additional fillers, all composites exhibited complete recovery of their macroscopic shape, forming transparent, self-standing films after reprocessing. However, subsequent drying at 120 °C under vacuum for eliminating any residual moisture affected the dimensional stability. Gels containing higher contents of NP-IL demonstrated superior shape retention and structural integrity after drying, while those with lower NP-IL or NP-UPy content displayed noticeable deformation or shrinkage. To further verify the effectiveness of the reprocessing process, broadband dielectric spectroscopy measurements were performed on the reprocessed gels. As shown in Fig. 6B, the temperature-dependent conductivity of the reprocessed G6 sample nearly overlapped with that of the pristine material, indicating that the ionic transport characteristics were fully restored. Thus, the dynamic crosslinking interactions enabled efficient reformation of the gel network without significant loss of electrochemical performance.
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| Fig. 6 (A) Reprocessing of G4, G6 and G7 via hot-pressing at 120 °C for 3 hours. (B) Conductivity as a function of temperature of G6 before and after reprocessing. | ||
Supplementary information (SI) is available. See DOI: https://doi.org/10.1039/d6py00098c.
Footnote |
| † H. H. and T. L. T. contributed equally to this work. |
| This journal is © The Royal Society of Chemistry 2026 |