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Thermal Resistance Jc⚠ unverified

Electrical / Power Electronics · Compute the junction-to-case thermal resistance

Parameters

InputSymbolUnitDefaultDescription
TjTjdegC1.0Junction temperature
TcTcdegC1.0Case temperature
PPW1.0Power dissipation
OutputSymbolUnitDescription
resultRthjcdegC/WJunction-to-case thermal resistance, in degrees Celsius per watt (degC/W). Returns positive infinity when ``P`` is not positive

The science & history

Understanding the Parameters

Derivation (Approaching a Proof)

Fourier heat conduction in one dimension gives $\Delta T = P\,R_{th}$ by analogy with Ohm's law ($V = IR$), where thermal resistance $R_{th} = L/(k A)$ for a slab of thickness $L$, conductivity $k$, area $A$. Defining the junction-to-case segment of that chain:

$$R_{\theta JC} \equiv \frac{T_j - T_c}{P}.$$

This is a definition of the effective resistance between those two thermal nodes under the test conditions used to measure it (usually a cold plate on the case). It does not by itself give $T_j$ in free air; you still need the rest of the thermal network and the same $P$.

Rearrangements used in design:

History

Thermal-resistance networks became standard semiconductor packaging language mid-20th century as power densities rose. JEDEC and manufacturer datasheets still quote $R_{\theta JC}$, $R_{\theta JA}$, and increasingly $\Psi_{JT}$ (junction-to-top characterization) for modern SMT power packages.

Related Concepts: Conduction Loss, Switching Loss, Temperature Rise, Efficiency Total, Diode Forward Loss

Notes: Registry calculator thermal-resistance-jc (unverified). Definitional steady-state model; transient thermal impedance $Z_{\theta JC}(t)$ is needed for pulses. Registry units use degC / degC/W (same as Celsius per watt).

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