Abstract
Glassy polymers are generally stiff and strong yet have limited extensibility1. By swelling with solvent, glassy polymers can become gels that are soft and weak yet have enhanced extensibility1,2,3. The marked changes in properties arise from the solvent increasing free volume between chains while weakening polymer–polymer interactions. Here we show that solvating polar polymers with ionic liquids (that is, ionogels4,5) at appropriate concentrations can produce a unique class of materials called glassy gels with desirable properties of both glasses and gels. The ionic liquid increases free volume and therefore extensibility despite the absence of conventional solvent (for example, water). Yet, the ionic liquid forms strong and abundant non-covalent crosslinks between polymer chains to render a stiff, tough, glassy, and homogeneous network (that is, no phase separation)6, at room temperature. Despite being more than 54 wt% liquid, the glassy gels exhibit enormous fracture strength (42 MPa), toughness (110 MJ m−3), yield strength (73 MPa) and Young’s modulus (1 GPa). These values are similar to those of thermoplastics such as polyethylene, yet unlike thermoplastics, the glassy gels can be deformed up to 670% strain with full and rapid recovery on heating. These transparent materials form by a one-step polymerization and have impressive adhesive, self-healing and shape-memory properties.
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Data availability
Data generated or analysed during this study are provided as Source data or included in the Supplementary Information. Further data are available from the corresponding author on request. More details on the methods are available in the Supplementary Information. Source data are provided with this paper.
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Acknowledgements
M.D.D. acknowledges support from the Coastal Studies Institute. We thank G. McKenna, Z. Bao, M. Balik and C. Bowman for their helpful discussions. S.S. and B.T.O. acknowledge support from NSF award no. 2324190. W.Q. is partially supported by Nebraska Research Initiative. All NMR measurements were made in the Molecular Education, Technology and Research Innovation Center (METRIC) at NC State University.
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Contributions
M.W., X.X. and M.D.D. conceived the idea. M.D.D. supervised the project. M.W. carried out most of the experiments. X.X. contributed to the SEM, transmittance test, adhesive demonstration and three-arm gripper design. X.X. and W.B. contributed to the FTIR measurement. S.S. and B.T.O. contributed to the dynamic mechanical analysis test. M.S. participated in the SEM measurement. E.F. participated in the Joule heating measurement. W.Q. contributed to the FTIR analysis. M.W., X.X. and M.D.D. wrote the paper, and all authors reviewed the paper.
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Extended data figures and tables
Extended Data Fig. 1 Comparison of three classes of polymeric materials.
a,b, Schematics (a) and tensile stress-strain curves (b) illustrating the role of identical solvent loading in gel and glassy gel. Adding solvent improves extensibility of glassy polymers, but usually weakens the mechanical properties (for example, hydrogel). In contrast, glassy gel is extensible like a gel, but stiff like the glassy polymer due to strong solvent-polymer interactions that non-covalently crosslink the polymer. Insets in b show individual tensile stress-strain curves. As an example, consider poly(acrylic acid) (PAA). In the absence of solvent, the polymer is glassy and stiff, yet brittle. Swelling in water produces a hydrogel (56 wt% water) that is many orders of magnitude softer, weaker, and extensible than the glassy polymer. In contrast, replacing water with an ionic liquid solvent (58 wt% ionic liquid) is nearly as stiff as a glass, while maintaining extensibility of a gel. c, A spider plot summary in terms of liquid content, toughness, recovery, fracture strength, and elongation. The experimental data is for PAA and the values in a are from tensile tests reported in b, c, and Supplementary Fig. 4.
Extended Data Fig. 2 Synthesis and properties of glassy gels.
a, Schematic illustration of the simple one-step approach to synthesize glassy gels from representative monomer (AA) and ionic liquid (PP). b,c, Transmission (b) and weight (c) changes of various gels. Inset in b shows photographs of various gels (thickness = 2 mm, diameter = 12 mm). Error bars on the data in c show standard deviation from three independent samples.
Extended Data Fig. 3 Glassy gels have multiple functions.
a, The ionic bonds give strong adhesion to surfaces despite being stiff and glassy (Middle: metal ball diameter from left to right: 0.25 inch, 0.5 inch and 1 inch). b, Heating-induced shape memory (width = 4 mm, length = 4.7 cm). The scale bar is 10 mm. c, Self-healing behavior. The gels merge together after healing at 80 °C for 60 s and are able to support a 500 g hanging weight. The diameter of the gel and the hole is 12 and 3 mm, respectively. In a-c, PAA-PP-6.0 M glass gel with a thickness of 1 mm is used.
Supplementary information
Supplementary Information
This file contains 20 Supplementary Figs. (chemical and mechanical characterizations, swelling, adhesion and conductivity tests, and application demonstrations), 3 Supplementary Notes (discussion of the toughening mechanism, multiple functions and application), 7 Supplementary Tables (composition and mechanical properties of various gels) and 10 Supplementary References.
Supplementary Video 1
The simple one-step synthesis of glassy gels. This video shows the simple one-step synthesis of the glassy gel. Note that as the glassy gel has excellent adhesive properties, a hydrophobic layer (ease release 200, Mann Release Technologies) was sprayed on the mould to remove the gel easily, making the glassy gel translucent.
Supplementary Video 2
Strong glassy gels. This video shows the high toughness of the PAA-PP-6.0 M glassy gel (0.156 g, cross-sectional area: 2 mm2) by lifting a 4 kg weight.
Supplementary Video 3
Recovery properties of the glassy gels. This video shows the excellent recovery of the glassy gel. Taking PAA-PP-6.0 M gel as an example, it was stretched to 350% strain and had a huge residual strain (324% strain). When elevating the temperature (that is, 80 °C), the residual strain can be fully recovered within 30 s.
Supplementary Video 4
Mixing of AA monomer and PP ionic liquid produces a strong exotherm. This video shows the exothermic behaviour of the AA and PP mix (Cm = 5.0 M, the volume of the mixture is 2 ml).
Supplementary Video 5
Adhesive properties of the glassy gels. This video shows the strong adhesion of the glassy gel. Taking PAA-PP-6.0 M gel as an example, it can hold stainless-steel metal balls (diameter: 0.25 inch, 0.5 inch and 1 inch) even when shaken vigorously, tilted vertically (shear) or flipped upside down (tension).
Supplementary Video 6
Shape memory properties of the glassy gels. This video shows the excellent shape-memory behaviour of the glassy gel. Taking PAA-PP-6.0 M gel as an example, it can be programmed fast and recovered rapidly. The glassy gel sample was stained red for visualization.
Supplementary Video 7
Self-healing properties of the glassy gels. This video shows the good self-healing property of the glassy gel. Taking PAA-PP-6.0 M gel as an example, the healed disc-shaped glassy gels (80 °C for 60 s) can hold a 500 g weight.
Supplementary Video 8
Glassy gel-based grippers by Joule heating. This video exhibits the performance of a heat-driven gripper composed of glassy gel (that is, PAA-PP-6.0 M) and liquid metals (LMs). The gripper can be easily softened by Joule heating by passing a current through the LMs. It can thereby grab and hold the object. Notably, a hydrophobic layer (ease release 200, Mann Release Technologies) was sprayed on the gel to eliminate strong adhesion so that the object could easily be released when cooled.
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Wang, M., Xiao, X., Siddika, S. et al. Glassy gels toughened by solvent. Nature 631, 313–318 (2024). https://doi.org/10.1038/s41586-024-07564-0
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DOI: https://doi.org/10.1038/s41586-024-07564-0
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