Dual-network (DN) conductive hydrogels consist of a rigid, brittle polymer network as the first network and a flexible, tough polymer network as the second network [
87]. The rigid network is typically crosslinked by covalent bonds, which act as sacrificial bonds, dissipating a significant amount of energy during large deformations, thereby maintaining the plasticity of the polymer network and preserving the integrity of the hydrogel [
69]. This approach addresses the poor mechanical performance and lack of rapid self-recovery and self-healing mechanisms found in conventional single-network ion-conductive hydrogels [
88,
89,
90]. For ion-conductive hydrogels containing conductive polymers, the conductive polymer chains typically serve the function of the first network, while the second network is often composed of flexible polymer chains such as PVA and PAM. For instance, Wang et al. [
91] reported dual-network conductive hydrogels where they incorporated polyaniline (PANI) into a poly (acrylamide-co-hydroxyethyl methacrylate) (P(AM-co-HEMA)) network via in situ polymerization. Due to the inherent interactions between the conductive PANI network and the flexible P(AM-co-HEMA), the prepared hydrogels exhibited excellent strength and toughness under cyclic loading. With an increase in the degree of PANI oxidation, both the mechanical properties and electrical conductivity of the hydrogels were enhanced. Additionally, soaking in salt solutions can enhance the electrical and mechanical properties of DN conductive hydrogels, as they are mutually influential. In the conductive hydrogels prepared by Zhou et al., hydroxypropyl cellulose (HPC) biopolymer fibers were physically crosslinked with a tough and biocompatible PVA gel matrix, followed by immersion in a salt solution to obtain ion-conductive hydrogels [
60]. The increase in HPC content resulted in higher tensile strength and stress of the conductive hydrogels, accompanied by an increase in electrical conductivity. This is attributed to the increased number of pores within the hydrogel, providing channels for the migration of salt ions, thus enhancing conductivity. Wei et al. [
92] utilized a method involving PVA pre-gels immersed in (NH4)2SO4 solution. This process induced PVA chain folding and precipitation due to the Hofmeister effect, resulting in ion-conductive hydrogels with a tensile strength of 4.1 MPa. In another study, dual-network ion-conductive hydrogels were created, incorporating sodium caseinate (SC) and PAM/carboxymethyl chitosan sodium (CMS-Na) [
93]. These hydrogels showcased outstanding mechanical properties and flexibility, utilizing the natural solubility of SC and its ability to spontaneously form micelle structures in water as energy dissipation centers. The in-situ synthesis of Ag/TA@CNCs within polyvinyl alcohol hydrogels to fabricate multifunctional nanocomposite hydrogels [
32] (
Figure 3i). These nanohybrids, such as LAPONITEs XLS (clay nanosheets), possess hydrophilicity and can be utilized as Nano-reinforcement materials and physical crosslinkers for synthesizing nanocomposite hydrogels with high tensile strength. This significantly enhances the hydrogel's elastic modulus, toughness, and extensibility (
Figure 3j,k). Additionally, ion-conductive dual-network hydrogels were achieved by immersing polyacrylamide/gelatin networks in sodium citrate solution [
94] (
Figure 3l). The ion crosslinking in the gelatin network served as reversible sacrificial bonds, absorbing energy during stretching and quickly reforming, thereby resulting in hydrogels with high mechanical performance (
Figure 3m,n). The network of nanocomposites is crucial in the realm of conductive hydrogels. This network can consist of exfoliated clay nanoparticles or simple fillers mixed within polymer matrices (such as carbon nanotubes, reduced graphene oxide, etc.). The uniform and continuous three-dimensional mesh structure grants hydrogels inherent flexibility and excellent mechanical properties. While conductive fillers in conductive hydrogels indeed enhance their electrical conductivity, their aggregation tends to disrupt the uniformity of the hydrogel structure, thereby compromising its mechanical performance. Incorporating conductive fillers into hydrophilic nanomaterials or modifying hydrophilic nanomaterials can significantly enhance the dispersibility of conductive materials. Consequently, incorporating nanocomposite materials into hydrogels can markedly improve their mechanical properties. For instance, incorporating oxidized multi-walled carbon nanotubes (oxCNTs) into polyacrylamide (PAM) hydrogel matrices enables the development of conductive nanocomposite hydrogels [
95]. By functionalizing oxCNTs, aggregation within the hydrogel network is circumvented, effectively enhancing the material's mechanical properties. The resulting hydrogel exhibits exceptional tensile performance and recyclability. Tondera and colleagues [
96] demonstrated that the synergistic interaction of nanoclay colloid dispersion with PEDOT and secondary polymer networks of polyacrylamide results in multi-network hydrogels with high electrical conductivity, stretchability, and printability. The excellent flexibility also relies on the intermolecular interactions within the hydrogel. Researchers have devised an exceptionally stretchable hydrogel by harnessing tannic acid-activated dynamic interactions (TEDIs) [
97], replacing conventional covalent cross-linking. The TEDI hydrogel exhibits a remarkable stretching capability exceeding 7300 %, which is 40 times that of chemically cross-linked hydrogels. Its potential in accurately detecting human motion for wearable electronic devices and healthcare monitoring, thus holding considerable application value. Additionally, Zhang et al. [
98] employed a one-pot synthesis method to develop a novel amphiphilic ionic liquid polymer hydrogel. By introducing acrylamide into the hydrogel composed of zwitterionic liquid and methacrylic acid lysine monomers, the hydrogel's strength is enhanced. The introduction of ZIL and lysine functional groups facilitates numerous non-covalent interactions (hydrogen bonds and ionic bonds) within the hydrogel. The outstanding mechanical properties of the Am-ZIL-LysMA hydrogel, with stretching exceeding 2000 %, demonstrate excellent stability, repeatability, and high strain sensitivity across a wide operating range.
Given the above considerations, different applications have varying requirements for the mechanical and electrical properties of conductive hydrogels. Conductive hydrogels used in electronic components demand high mechanical conductivity and electrical conductivity. Conversely, those utilized in sensors may not require high electrical conductivity but place significant emphasis on properties such as stretchability, compressibility, and flexibility. Therefore, in practical applications, there needs to be a balance between mechanical conductivity and electrical conductivity, tailored to the specific requirements of each application.