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Rθ network · Tj = Ta + P·Σθ · margin to Tj,max

Junction Temperature Console

Heat flows out of the silicon through a series of thermal resistances — junction-to-case, the interface material, then the cooler to air. Junction temperature is ambient plus power times the sum of those resistances. Compute Tj and every node temperature, and check the margin to the chip's maximum.

01 · Quick estimate

Power, ambient & thermal resistances → junction temperature.

Junction temp
130°
-25°C to Tj,max
Resistance stack & node temperatures ↓
02 · Deep analysis

Thermal chain console

Resistance stack
Thermal resistance stack: junction to sink temperatures130°CJunction (Tj)95°CCase74°CSinkambient · heat flows down to air
130°/ 105°C
Junction temp
130°C
Margin to max
-25°C
Total θ j-a
0.150
°C/W
Total rise
105°C
over ambient
Where the heat builds · rise per resistance
Cooler (sink→air)+49°C
Interface (case→sink)+21°C
Package (junction→case)+35°C

The largest bar is your best lever. The cooler (θsa) usually dominates — liquid cooling slashes it.

Over limit · 130°C vs 105°C max

Junction hits 130°C — 25°C over the limit. Lower the cooler resistance (liquid cooling), improve the TIM, or reduce power.

Get the interface term θcs from the TIM Calculator; check hotspot flux in the Power Density console.

Why it matters

Why the resistance chain governs everything

Junction temperature is a series of resistances

Heat flows junction → case → interface → sink → air, each step a thermal resistance (°C/W). Tj is ambient plus power times the sum of those resistances — a simple, exact chain that governs whether a chip survives.

Most designs live or die at the sink-to-air step

The cooler's resistance (sink-to-ambient) is usually the largest and the one you control. Air cooling has high resistance; liquid cold plates slash it, which is the single biggest lever on junction temperature for high-power parts.

There's always a Tj,max you can't cross

Every chip has a maximum junction temperature (often ~105°C) above which it throttles or degrades. Thermal design is the discipline of keeping Tj below that limit with margin across the worst-case ambient and power.

θ adds, so every layer matters

Because resistances sum, a great cooler can be undone by a poor thermal interface, and vice versa. The whole chain has to be good — which is why TIM choice, lid, and cooler are co-designed.

Field notes

Ohm's law for heat

Junction temperature is the single number that decides whether a chip runs or throttles, and the beautiful thing is how simply it's governed. Heat behaves like current and temperature like voltage, so the path from the silicon to the air is just a chain of resistances in series, and the temperature rise across the chain is the power (the ‘current’) times the total resistance. Junction temperature is ambient plus that rise: Tj = Ta + P × Σθ. That's Ohm's law for heat, and it's exact.

The chain has three links you control to different degrees. The junction-to-case resistance is fixed by the package — the chip vendor's problem, not yours. The case-to-sink resistance is the thermal interface material, a thin but critical layer where a bad choice can cost tens of degrees. And the sink-to-ambient resistance is the cooler, usually the largest term and the one you most directly choose — which is why moving from air to a liquid cold plate, slashing that resistance, is the most powerful thermal lever available.

Because the resistances add, the chain is only as good as its worst link. A magnificent cold plate is wasted behind a thick, cheap thermal pad; a superb interface material can't save an undersized heatsink. This is why thermal design is holistic — the package, the TIM and the cooler are co-designed, and the rise-per-resistance breakdown in this console shows you exactly which link is costing you the most degrees, so you spend effort where it pays.

Two cautions. Ambient is one-for-one: a design comfortable at 25°C can fail at a 40°C datacenter inlet, so always check the worst-case ambient. And this is a steady-state model — correct and conservative for sustained AI workloads, but bursty loads need transient analysis. Bring the interface resistance from the TIM Calculator, and for parts with concentrated hotspots, complement this with the Power Density console.

Junction Temperature FAQs

Have more questions? Contact us

Trusted by Thermal Design & Reliability Teams

4.8
Based on 3,120 reviews

The node-by-node temperature breakdown — sink, case, junction — is exactly how I diagnose a thermal chain. Showing that a great cold plate is wasted behind a thick TIM, because the resistances add, is the lesson juniors need. The presets match our reference designs.

D
Dr. Helena Vossberg
Thermal design engineer
June 2, 2026

Tj = Ta + P·Σθ done right, with the margin to Tj,max front and center. I use it to size the cooler resistance budget before picking hardware. The ambient-sensitivity point is the one that bites real deployments at 40°C inlet.

R
Rajesh Pillai
Server cooling architect
April 22, 2026

Clean, exact, and honest about steady-state vs transient. The Tj,max margin verdict is what our sign-off hinges on. Pairs perfectly with the TIM calculator for the interface term — bring θcs over and see the chain.

M
Mia Sørensen
SoC reliability
March 2, 2026

Great for quick thermal-budget checks. The resistance-stack visualization makes the series-resistance idea click. Would love a transient impedance curve, but for steady-state cooling sizing it's spot on.

C
Caleb Owusu
Hardware engineer
December 29, 2025

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Tj = Ta + P × (θjc + θcs + θsa) · steady-state thermal-resistance network · Last reviewed: 2026-06