RadiatorTemp

Coolant temperature a loop settles at, the fan speed a target temperature needs, and optionally the noise at that speed.

Loop

Fans (one per 120 / 140 mm)

Heat

Result

Coolant–
Above intake air–
Dissipation–
Airflow through core–
Target coolant –

Method

A radiator moves heat in proportion to the difference between coolant and incoming air: Q = q · (Tcoolant − Tair). Solving for the coolant gives the equilibrium. q is the dissipation in W/K.

q depends on the air actually passing through the core, not on fan rpm as such. Airflow per fan is CFMmax · derate · rpm/rpmmax with the radiator derate from the airflow tool (0.62, or 0.72 for pressure-optimized blades, ×1.12 push-pull, less for thicker cores). Per 120 mm segment at 27 mm: q = 8.5 W/K · (airflow / 45 CFM)0.6. Heat transfer over fins scales with roughly the 0.6 power of velocity.

CoreAirflow factorFin area factorNet at same rpm
22 mm1.060.930.96
27 mm1.001.001.00
38 mm0.901.151.08
45 mm0.841.221.10
60 mm0.761.301.10

Thick cores gain fin area but lose airflow; at low rpm the net is close to zero. With fans off, natural convection is taken as 1 W/K per segment.

The band is ±15 % on q: fin density, coolant flow and preheated case air. Pump speed matters little above roughly 1 l/min.

Die temperatures sit above the coolant by the block and TIM delta, typically 25 to 45 K under load.

Noise, if a dB(A) rating is given: Lmax + 50 · log₁₀(rpm/rpmmax) added on an energy basis to a 6 dB(A) motor and bearing floor, plus 10 · log₁₀(fan count). Same model as the noise tool.