Conductor Resistance Temperature Correction
Also known as temperature coefficient of resistance
Worked example: 10 Ω copper, 20 °C → 75 °C gives 12.1615 Ω — press Try an example to run it live, then adjust anything.
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Conductor Resistance Temperature Correction explained
Metals conduct worse when hot: heat jostles the lattice and scatters the electrons. Copper's coefficient is about 0.00393 per kelvin referenced to 20 °C, aluminium's about 0.00403, so a 10 Ω copper winding at 20 °C measures 10 × (1 + 0.00393 × 55) = 12.16 Ω at 75 °C — a 22% rise. Because a kelvin and a Celsius degree are the same size, only the temperature difference matters; if your α is quoted per °F, choose that unit and the solver handles it.
This relation is quietly one of the most useful in the trade. It turns a winding's cold and hot resistance into a motor's average winding temperature, the basis of the standard heat-run test — no thermocouple can reach the middle of a coil, but its resistance always can. It is also why cable ampacity tables assume a conductor temperature, why voltage-drop constants differ between 20 °C and 75 °C, and why platinum's clean, repeatable version of this curve makes the RTD the workhorse of industrial temperature measurement.
Conductor Resistance Temperature Correction formula
- = Resistance at T₂ (Ω)
- = Resistance at T₁ (Ω)
- = Temperature coefficient (1/K)
- = New temperature (°C)
- = Reference temperature (°C)
Missing one of these? Work it out first, then come back
- Resistance at T₂ — Series RLC Impedance, Series RL or RC Impedance
- Resistance at T₁ — Series RLC Impedance, Series RL or RC Impedance
- Temperature coefficient — PV Temperature Derate, Thermal Linear Expansion
- New temperature — Ideal Gas Law, Antoine Equation (Vapour Pressure)
- Reference temperature — F-Value (Equivalent Time at Reference Temperature), Nurse-Saul Equivalent Age