with exceptional mechanical resilience, self-healing properties, and processability have been reported recently. [16] Although hydrogel composites remain useful materials for sensor and biomedical applications, broad use is restricted by their operating temperature range (0−100 °C), long-term stability, and the need for watersoluble reagents.Conductive organogel composites have received comparatively little attention despite the ability to support a wide range of polymers and fillers, exhibit conductivities between 10 −4 and 10 mS cm −1 , [17] and maintain useful mechanical and electrical properties at temperature extremes without solvent evaporation or freezing. [18] Furthermore, the synthetic tunability of organogels provides access to a diverse range of materials. For example, dynamic organogels can be synthesized with reversible covalent bonds or secondary interactions such as hydrogen bonding to facilitate self-healing, network reversion, or sensing capabilities. [19][20][21][22][23][24][25][26][27] Variability in solvent, polymer, and filler selection allows access to materials mimicking the mechanical properties of hydrogel composites and soft conductive elastics, and enables performance inaccessible to either system alone such as stimuli responsivity and temperature stability. Recyclable hemiaminal dynamic covalent networks (HDCNs) formulated with insulating polyethylene glycol (PEG) and conductive fillers present advantages in applications such as pressure and chemical sensors, antistatic technologies, and other flexible electronics. [27][28][29][30][31][32] A survey of conductive nanoparticles was added to HDCN organogels during their synthesis in N-methyl-2-pyrrolidone (NMP): "long" (10 µm × 12 nm) multi-walled carbon nanotubes (MWCNTs), four types of carbon black (Black Pearls L (BPL), 9A32, XC72, XC72R), and graphite. Microscale behaviors were first established through rheology. HDCN composites remained in a dynamic state, underwent stress relaxation up to 2 h after formation, and had relaxation stretching parameters close to zero (β = 0.01−0.09, R 2 ≈ 0.95, Table S1, Supporting Information), independent of solvent and filler choice. The stretched relaxation behavior was attributed to hierarchical and continuous segmental relaxation from the dynamic heterogeneity of transient networks. Transient covalent crosslinks and supramolecular interactions are active throughout the gel at various length scales and stages of relaxation, changing the kinetics of chain motion as a function of their fluctuation, and creating a wide distribution of relaxation behaviors over long time periods. [33][34][35][36][37] Notably, β values for composites were comparable to the matrix alone (β = 0.02), suggesting uniform filler
Conductive OrganogelsAs the use of automation in industry accelerates, the development of flexible, electrically conducting materials with the requisite environmental resilience for impact-resistant sensors, foldable electronics, and electrostatic shielding are needed; simultaneously, recyclability fo...