2020
DOI: 10.1039/d0sm01094d
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Network topologies dictate electromechanical coupling in liquid metal–elastomer composites

Abstract: Conductive traces of elastomer embedded with liquid metal droplets exhibit little change in electrical resistance when stretched to large strains. Computational modeling is performed to better understand this remarkable piezoresistive property.

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Cited by 48 publications
(54 citation statements)
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“…Moreover, the low q scattering curve of the microfiber at 0% strain shows a q −3.5 scattering, which shifts to q −3.0 at 300% strain, indicating the loss of fiber density after stretching as LM particles start to flow. All the above observations coincide with the recent computation results from Zolfaghari et al ( 54 ) who explained the reduced electromechanical coupling of LM-embedded elastomers to mainly two principal contributions: One is the hydrostatic pressure–controlled opening of the narrow, neck-like connections among LM droplets, and the other one, probably the primary contribution, is the stretching out of the original highly tortuous serpentine conductive path, which does not prominently alter their length and average cross-sectional area to preserve the end-to-end conductance ( G = σ A / l ; where σ is the intrinsic conductivity of LM, A is the cross-sectional area, and l is the conductive length). A schematic mechanism for the strain-insensitive conductance of LM sheath-core microfiber is presented in fig.…”
Section: Resultssupporting
confidence: 93%
“…Moreover, the low q scattering curve of the microfiber at 0% strain shows a q −3.5 scattering, which shifts to q −3.0 at 300% strain, indicating the loss of fiber density after stretching as LM particles start to flow. All the above observations coincide with the recent computation results from Zolfaghari et al ( 54 ) who explained the reduced electromechanical coupling of LM-embedded elastomers to mainly two principal contributions: One is the hydrostatic pressure–controlled opening of the narrow, neck-like connections among LM droplets, and the other one, probably the primary contribution, is the stretching out of the original highly tortuous serpentine conductive path, which does not prominently alter their length and average cross-sectional area to preserve the end-to-end conductance ( G = σ A / l ; where σ is the intrinsic conductivity of LM, A is the cross-sectional area, and l is the conductive length). A schematic mechanism for the strain-insensitive conductance of LM sheath-core microfiber is presented in fig.…”
Section: Resultssupporting
confidence: 93%
“…[ 10,11,17,21 ] This coupling is likely a function of the morphology of the percolation network, [ 11 ] and we are involved in ongoing work on modeling and characterizing the droplet morphology as it relates to electromechanical coupling. [ 36 ]…”
Section: Figurementioning
confidence: 99%
“…For traditional conductive materials, the relative increase in electrical resistance can be predicted by the Pouillet's law: Δ Ω / Ω 0 = λ 2 − 1 (λ is the stretched times). [ 38 ] The inset figure is the change of normalized electrical resistance of our composite at different strains compared with Pouillet's law. The stress−strain curve of the SBS&LM@MUA composite shows that increasing LM will reduce the strength of SBS&LM@MUA composite (Figure 4f).…”
Section: Resultsmentioning
confidence: 99%