The electrode drives radio-frequency current through the tissue; resistive (Joule) heating deposits power in a small volume under the tip, and that heat then diffuses outward. The grid solves the 2D heat equation explicitly at every frame:
∂T/∂t = D·∇²T − k·(T − T_body) + Q(x,y,t)
D = thermal diffusivity of tissue
k = perfusion/convective cooling toward T_body ≈ 37°C
Q = electrode power deposited under the tip,
weighted by distance from the contact point
Tissue response is threshold-driven, not linear — the same physics real electrosurgeons watch for:
- ~45–60 °C — hyperemia, reversible if it stops here.
- ~60–70 °C — protein (collagen) denaturation: the tissue visibly whitens. This is the coagulation/sealing window.
- ~100 °C — intracellular water flashes to steam; the tissue desiccates.
- >150 °C — carbonisation (char); charred tissue is a poor conductor, so power stops coupling efficiently and further cutting stalls.
Cut mode concentrates power into a small, high-intensity spot that reaches vaporisation almost instantly, mechanically parting tissue (the block visibly grooves and blackens). Coagulate mode spreads a lower, wider power over a longer dwell so more tissue volume passes through the 60–70 °C denaturation window without ever reaching char — the goal when sealing a bleeding vessel. Hold the tip over a red vessel marker in Coagulate mode; if it stays in the sealing window long enough it turns solid (sealed). Overheat it past ~160 °C and it chars instead — a real failure mode called an inadequate or "burnt" seal.