Rui
Zhang
*a,
Hengzhi
Ruan
a,
Qionglong
Fu
a,
Xuedong
Zhu
*a and
Yuan
Yao
*b
aEngineering Research Center of Large Scale Reactor Engineering and Technology, Ministry of Education, School of Chemical Engineering, East China University of Science and Technology, 130 Meilong Road, Shanghai 200237, China. E-mail: r.zhang@ecust.edu.cn; xdzhu@ecust.edu.cn
bSchool of Materials Science and Engineering, East China University of Science and Technology, 130 Meilong Road, Shanghai 200237, China. E-mail: yaoyuan@ecust.edu.cn
First published on 18th May 2020
A fully physically linked poly(acrylic acid) (PAA) hydrogel with temperature sensitivity was fabricated. The temperature-sensitive point of the hydrogel was near 25 °C when introducing the copolymer of N-isopropylacrylamide (NIPAAM) and dopamine methacrylamide (DMA). More importantly, the hydrogels exhibited excellent self-healing properties, mechanical properties and tunable adhesive strength and could be used as epidermal sensors.
Fig. 1 shows a general procedure to prepare PAA/NIPAAM-co-DMA hydrogels. Briefly, the hydrogel was prepared by free-radical polymerization of AA in H2O in the presence of copolymer NIPAAM-co-DMA, which was synthesized as following (Scheme S1, ESI†). When the temperature was low, the hydrogen bonding in the network was enhanced due to the carboxyl group of PAA, phenolic hydroxyl group of DMA and acylamino group of PNIPAAM. However, when the temperature was increased, the copolymer NIPAAM-co-DMA was transformed due to the hydrophobic effect of isopropyl of NIPAAM and side chain groups of DMA, so the copolymer NIPAAM-co-DMA formed many hydrophobic regions that helped to dissipate excess energy. And this phenomenon could also be observed in the pre-gel solution; the solution changed from transparent to opaque white when the temperature increased.
Fig. 2a and b show the typical tensile stress–strain curves and toughness of hydrogels at different temperatures. For PAA hydrogels, no obvious thermal response was observed at different temperatures. In contrast, the fracture stress and toughness of PAA/NIPAAM-co-DMA gels were influenced by the increase of temperature dramatically. DSC thermograms of PAA/NIPAAM-co-DMA hydrogels during heating was provided in Fig. S3 (ESI†). In the previous research studies, cyclic tensile loading–unloading tests were performed to study the toughening mechanism of sacrificial bonds, and the hysteresis indicates the amount of energy dissipated.34Fig. 2c shows the stress–strain curves after consecutive loading–unloading cycles and illustrates the energy dissipation capacity of the PAA/NIPAAM-co-DMA gels, which was another indicator to assess the mechanical properties of the obtained hydrogels. It could be seen that the hysteresis did not become much smaller when the subsequent cycle was conducted immediately after the previous cycle. In addition, no energy hysteresis phenomenon was observed during the cyclic tensile loading–unloading tests. Simultaneously, the dissipated energy of loading–unloading cycles was calculated, as shown in Fig. 2d. It was clear that no obvious decrease of dissipated energy appeared as the cycle number increased and the average dissipated energy was about 650 kJ m−3, which was larger than that of other hydrogels based on hydrophobic interactions35 and this indicated the excellent fatigue resistant properties of PAA/NIPAAM-co-DMA gels. Interestingly, we found that the obtained hydrogels could be stretched to 15 times with a cut notch (radius ≈ 2 mm) (Fig. 2e). As shown in Fig. 2f, the notch was blunted and remained stable during the whole testing process, suggesting that no stress concentrates in the front of the notch tip.
Because of the supramolecular interactions in the network, physically linked hydrogels usually show excellent self-healing ability.36 As illustrated in Fig. 3a, the hydrogel was cut into two pieces that were dyed red and blue. Then, they were brought together and left to heal at room temperature without any stimulus. After 16 h, the line at their interface was blurred, which indicated that the interactions in the hydrogel system were dynamic. To investigate whether the intermolecular noncovalent bonds in the PAA/NIPAAM-co-DMA gels dissociate and reassociate efficiently under stress, mechanical tests were performed on the obtained hydrogels. Fig. 3b shows the stress–strain curves of healed hydrogels with different NIPAAM-co-DMA concentrations. The corresponding healing efficiency of the healed hydrogels is demonstrated in Fig. 3c; it indicates that the healing efficiency decreased from 69.76% to 58.14% when the NIPAAM-co-DMA concentration was improved from 1.2% to 2.2%. Another phenomenon shown in Fig. 3d and e was that the efficiencies of the hydrogels were enhanced with the increase of the healing time. Due to the inadequate recovery in the network, the hydrogel was broken at λ = 7 after healing for 8 h. Meanwhile, after healing for 24 h, the healing efficiency and ultimate strain of the hydrogel were about 92.31% and 4880%, which was very close to the strain of the origin hydrogel (λ = 51) (Fig. S4, ESI†). The self-healing property of PAA/NIPAAM-co-DMA gels was related to the dynamic hydrogen bonds that were formed between PAA and NIPAAM-co-DMA. When the hydrogel was broken under stress, the hydrogen bonding could be reformed at room temperature between the fresh cross-section. Simultaneously, the mobility of the polymer chains was also responsible for the process of self-healing. The reason was that the higher the density of crosslinking, the more difficult it was for PAA and NIPAAM-co-DMA chains to move.37 When the NIPAAM-co-DMA concentration was too high, very few chains could move from one surface to another surface leading to a poor healing performance.
In all, four main noncovalent interactions, including hydrophobic, ionic electrostatic, van der Waals interactions, and hydrogen bonding have been reported in building high strength hydrogels.38 Due to the reversible nature of these interactions, physical gelation commonly tends to be brittle and weak when a force is applied.39 To design an adhesive hydrogel with outstanding mechanical properties, DMA was introduced into the system to improve the balance between cohesion and adhesion. In order to display the adhesive performance of PAA/NIPAAM-co-DMA gels intuitively, pictures of hydrogels adhering to various materials are shown in Fig. 4a. It was worth noting that the obtained sample exhibited excellent adhesive behavior when it was adhered to paper, copper, steel, skin, glass and plastic and it could even withstand a 100 g weight, as shown in Fig. 4a. In addition to revealing the adhesion strength of the gels, a combinatorial study of the effect of NIPAAM-co-DMA concentration and temperature is shown in Fig. 4b. For all the samples, the adhesion strength was dramatically influenced by the NIPAAM-co-DMA content. For example, the adhesion strength of the hydrogels at 15 °C improved from 340 KPa to 543 KPa when the concentration of NIPAAM-co-DMA was increased from 1.2 wt% to 2.2 wt%. It could be concluded that addition of catechol group contents led to more interactions at the adhesion interface. Meanwhile, adhesion experiments of PAA/NIPAAM-co-DMA gels at different temperatures were also conducted. We found that the samples at 25 °C, which was close to the temperature-sensitive point of the hydrogels (Fig. S3, ESI†), showed the lowest adhesion strength compared to other temperatures. Furthermore, when the temperature was increased to 35 °C, for instance, the adhesion strength of PAA0.5DN0.017 gels increased from 315 KPa to 480 KPa. A similar phenomenon was also observed in other samples that could be attributed to two reasons. First, as the temperature was increased above the temperature-sensitive point, DMA chains became hydrophobic, allowing the expulsion of water molecules and acting like other poly(NIPAAM)s.40 As a result, hydrogen bonding at the adhesion interface was impaired, thus adhesion performance became hampered. Second, when the temperature was higher than room temperature, water content in the samples decreased quickly leading to stronger interactions in the system and hydrogels exhibited higher adhesion strength.
Due to the excellent mechanical properties and adhesive ability, the PAA/NIPAAM-co-DMA gel could be used as an epidermal sensor in the presence of lithium chloride. As shown in Fig. 5a–c, the monitored resistance of the PAA/NIPAAM-co-DMA gel-based sensor could accurately reflect the finger motion at different angles, indicating the sensing reliability of the PAA/NIPAAM-co-DMA gel-based sensor. Moreover, the relationship between the relative resistance of the PAA/NIPAAM-co-DMA gel-based sensor and strain is consistent with the result in Fig. 5d. As the sensor was stretched, the relative resistance increased and this demonstrated the stability of the sensor under an external force. We ascribed the sensitivity of the PAA/NIPAAM-co-DMA gel-based sensor to the free ions such as H ion and residual initiator in the hydrogel network and therefore the gel was conductive.
In conclusion, we developed a temperature-sensitive and tough hydrogel of a fully physically linked PAA/NIPAAM-co-DMA gel, with adhesive strength and self-healing ability. The hydrogel exhibited excellent fatigue resistance and crack resistance properties and could be used as an epidermal sensor. According to DSC and rheological investigation, the temperature-sensitive point of the hydrogels was near 25 °C. Our design strategy will open up a new platform to overcome the limitation of conventional hydrogels that are brittle and weak and makes progress in the preparation of functional materials.
This work is supported by the National Natural Science Foundation of China (21374029, 51573088 and 21776076).
Footnote |
† Electronic supplementary information (ESI) available: For experimental methods and other characterization of the hydrogels, see DOI: 10.1039/d0ma00282h |
This journal is © The Royal Society of Chemistry 2020 |