2026-04-28
Every power circuit wastes some energy as heat. If you don't manage that heat, your components derate, drift, or die. Thermal design isn't an afterthought — it's a core part of your circuit working reliably.
The Thermal Model: Think Like an EE
Heat flow follows an analogy to Ohm's law. Power dissipation (P) is your "current," temperature difference (ΔT) is your "voltage," and thermal resistance (Rθ) is your "resistance." The fundamental equation is:
Tjunction = Tambient + P × RθJA
where RθJA is the total thermal resistance from the silicon junction to ambient air, measured in °C/W. Every datasheet lists this. Chain multiple thermal resistances in series just like resistors: RθJA = RθJC + RθCS + RθSA (junction-to-case, case-to-sink, sink-to-ambient).
Concrete Example: A Linear Regulator
You're dropping 12V to 5V at 500mA using an LM7805 in a TO-220 package. The power dissipated is:
P = (12V − 5V) × 0.5A = 3.5W
The LM7805 in TO-220 has RθJA ≈ 65°C/W without a heatsink. At 25°C ambient, the junction temperature would be 25 + 3.5 × 65 = 252°C — far above the 150°C maximum. The part will shut down or fail.
Adding an aluminum heatsink with RθSA = 10°C/W and using a thermal pad (RθCS ≈ 1°C/W), with RθJC = 5°C/W for the TO-220:
TJ = 25 + 3.5 × (5 + 1 + 10) = 25 + 56 = 81°C — well within limits.
Practical Rules of Thumb
When choosing packages, note that a SOT-223 (RθJA ≈ 60°C/W with a good pad) handles about 1.5W before needing help, while a QFN exposed pad can manage 2–3W with proper PCB design. Always run the junction temperature calculation before committing to a package.
