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Peng et al. Soft Sci 2023;3:36  https://dx.doi.org/10.20517/ss.2023.28           Page 5 of 12

               The mechanism of conductive pathway formation in the magnetic LME is shown in Figure 1C. Initially, the
               LM ferrofluid microparticles are evenly distributed in the elastomer precursor solution. Under the magnetic
               field, the LM ferrofluid particles aggregate to connect to form continuous conductive networks at the
               composite bottom. We then cured the elastomer to form an initially conductive LME that can maintain
               high conductance stability when stretched.

               The magnetic LME composites also show printability, allowing us to print various functional electronic
               components, such as micro-circuit chips [Figure 1D], patterned stretchable circuits [Figure 1E], and
               multilayer circuits. Furthermore, owing to the excellent thermal conductivity and thermal stability of the
               LM ferrofluid, the conductive LME composite can be embedded in temperature-responsive hydrogel
               actuators to achieve wireless induction heating [Figure 1F].


               Preparation and characterization of conductive LME composite
               The preparation of the conductive LME composite is schematically depicted in Figure 2A, and the details
               are provided in the Experimental Section and Supplementary Table 1. In a typical operation, we dispersed
               the LM ferrofluid to the Ecoflex 0030 part A by mechanical stirring. We observed the solution changed from
               colorless to opaque grey-black during the stirring. This is due to the formation of LM ferrofluid particles
               under the shear force. After mixing with the Ecoflex 0030 part B, we applied the magnetic field to the
               solution to attract LM ferrofluid microparticles to the composite bottom [Figure 2B]. The magnetic
               aggregation can increase the local concentration of LM ferrofluid particles and reduce the distance between
               the particles. Therefore, the LM ferrofluid particles tend to connect to form continuous conductive
               networks.


               We also found the LM ferrofluid cannot maintain its ellipsoidal shape compared to the pure LM [Figure 2C
               and Supplementary Figure 3A]. To further explore the properties of the LM ferrofluid, we performed the
               contact angle and surface tension tests [Supplementary Figure 3B]. The results show that the contact angle
               and the surface tension of the LM ferrofluid were lower than those of the pure LM [Figure 2D]. We also
               compared the particle distribution in the composite before and after applying the magnetic field. For the
               composite without applying the magnetic field, the LM ferrofluid microparticles are uniformly dispersed in
               the elastomer matrix [Supplementary Figure 4]. For the one with magnetic aggregation, the composite
               exhibits the Janus structure with high stretchability [Figure 2E and F]: the upper insulative layer was in light
               grey with a low concentration of LM particles, while the lower conductive layer was grey and black with
               highly condensed magnetic LM particles.


               Under the magnetic field, the LM ferrofluid microparticles aggregated at the bottom of the elastomer
               matrix. Since LM ferrofluid particles are almost incompressible, the magnetic force induces the LM
               ferrofluid droplets to merge by breaking the oxide layer of the LM [Supplementary Figure 5]. The SEM
               image shows the distribution of LM ferrofluid particles is increased from the top to the bottom, and the
               particles coalesce into a continuous conductive pathway at the bottom [Figure 2G]. We also used 3D micro-
               CT tomography to study the microstructure of the composite. We found that the denser LM ferrofluid
               droplets were aggregated at the bottom while the low-density elastomer matrix was concentrated at the top
               [Figure 2H]. SEM and corresponding EDS analysis further show that Cu@Fe microparticles were wrapped
               by LM in the composite [Figure 2I and J]. Our proposed magnetic aggregation method can activate the
               conductive filler networks before the elastomer curing without the post-sintering operation. Therefore, this
               approach can overcome the limitations of mechanical sintering on the hardness of the matrix, as the soft
               elastomer matrix (Ecoflex) cannot provide strong mechanical support for sintering.
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