1.1 Core Mechanism of Silicone Thermal Conductivity
Thermal conductive rubber is a functional material created by filling a rubber matrix with thermally conductive fillers, balancing thermal conductivity, insulation, and elasticity:
Property
Advantage
Thermal Path Construction
Fillers (Al₂O₃/BN/graphene) form conductive networks for directional heat dissipation
Volume resistivity >10¹² Ω·cm, breakdown voltage >10 kV/mm
Environmental Resistance
Temperature range: -60°C~250°C, UV/ozone/chemical corrosion resistance
Silicone rubber itself is a poor thermal conductor (inherent conductivity: 0.1-0.3 W/m·K). Its thermal performance entirely depends on filler system design:
Phonon-Dominated Heat Transfer: Heat propagates through non-metallic materials as lattice vibration waves (phonons). Silicone’s disordered molecular chains scatter phonons, while highly conductive fillers (e.g., AlN, diamond) establish efficient phonon pathways via regular crystal structures.
Filler Network Construction: When filler volume fraction exceeds 70%, particles form interconnected 3D thermal networks, enabling rapid heat transfer along “filler chains”.
Interfacial Thermal Resistance Optimization: Silane coupling agents modify filler surfaces, enhancing chemical bonding with silicone and reducing phonon scattering losses at interfaces (thermal resistance reduced by up to 50%).
Silicone remains the optimal choice due to its molecular chain flexibility, wide temperature tolerance (-50~200°C), and high filler tolerance (>90% filler content while maintaining elasticity). Other rubbers serve only as limited-scenario alternatives with significantly higher costs.
1.2 Feasibility of Thermal Conductivity in Other Rubbers
Thermal conductivity isn’t exclusive to silicone, but other rubbers face three major challenges: