Le S2. The sequence of the influence P3HT with unique molecular weights on on the

Le S2. The sequence of the influence P3HT with unique molecular weights on on the thermal conductivity of GNS@P3HT of P3HT with distinctive molecular weights the thermal conductivity of GNS@P3HT membranes was was as GNS@P3HT (6000)/PVDF, GNS@P3HT (2000)/PVDF, GNS@P3HT membranes as follows:follows: GNS@P3HT (6000)/PVDF, GNS@P3HT (2000)/PVDF, (ten,000)/PVDF, GNS@P3HTGNS@P3HT (14,000) /PVDF, and GNS/PVDF. The in-plane GNS@P3HT (ten,000)/PVDF, (14,000) /PVDF, and GNS/PVDF. The1in-plane thermal con- -1 ductivity with the GNS@P3HT (6000)/PVDF membrane membrane was four.17 W m-1 loading thermal conductivity on the GNS@P3HT (6000)/PVDFwas four.17 W m K at a fillerK-1 at a of 20 wt , which wt , which greater than greater than that of pure PVDF. conductivity filler loading of 20 was 26 timeswas 26 instances that of pure PVDF. The thermal The thermal of the GNS@P3HT membrane membrane was considerably higher than that membrane. conductivity from the GNS@P3HT was drastically greater than that on the GNSof the GNS The GNS Propidium In Vivo modified by P3HT with distinctive molecular weights could have already been uniformly membrane. The GNS modified by P3HT with diverse molecular weights could have dispersed and oriented in PVDF, which NADPH tetrasodium salt Technical Information formed a dense thermal conductivity pathway of been uniformly dispersed and oriented in PVDF, which formed a dense thermal conducPVDF membranes [37]. Simultaneously, the interface thermal resistance among GNS was tivity pathway of PVDF membranes [37]. Simultaneously, the interface thermal resistance lowered, which, in turn, enhanced the thermal conductivity from the membrane. Also, between GNS was reduced, which, in turn, improved the thermal conductivity in the the thermal conductivity of GNS@P3HT (6000)/PVDF was the highest relative for the modmembrane. Moreover, the thermal conductivity of GNS@P3HT (6000)/PVDF was the ified graphene membranes of other P3HT molecular weights. Compared with the other highest relative to the modified graphene membranes of other P3HT molecular weights. three modified molecular weights, the P3HT chain using a molecular weight of 6000 g/mol Compared using the other three modified molecular weights, the P3HT chain with a moformed a hugely matched structure on the surface of GNS when the chain interacts with lecular weight of 6000 g/mol formed a extremely matched structure around the surface of GNS GNS via interaction, which was effective for the transfer of phonons involving when the chain interacts with GNS by way of interaction, which was effective for the GNS sheets and decreased the scattering for the duration of phonon transfer. Nevertheless, the excessive transfer of phonons amongst GNS sheets and decreased the scattering through phonon transmolecular chains could be stacked within a somewhat disorderly manner around the surface of fer. Nevertheless, the excessiveinteraction chains could beand GNSin athis region, disorderly GNS, resulting in a weak molecular between P3HT stacked in somewhat that will manner on the surface of GNS, resulting in a weak interaction GNS. Hence, the GNS in greatly hinder phonon transmission via P3HT to nearby involving P3HT and thermal this area, whichcomposites of P3HTphonon transmission by means of P3HT to nearby GNS. conductivities of will tremendously hinder modified graphene with distinctive molecular weights As a result, diverse. Also, the thermal percolation threshold of PVDF composites with had been also the thermal conductivities of composites of P3HT modified graphene with distinctive molecular weights had been also differe.