R = ρ · L / A
Long, thin conductors have higher resistance; material and temperature determine ρ.
Long, thin conductors have higher resistance; material and temperature determine ρ.
Select a target and calculate.
Long, thin conductors have higher resistance; material and temperature determine ρ.
10 m of 10 mm² copper: 0.0175 Ω.
DC, constant temperature and homogeneous cross-section.
This calculator finds the missing quantity among conductor resistance R, resistivity ρ, conductor length L and cross-sectional area A from the other three. It shows why long, thin cables can cause noticeable voltage drop at high currents, and why a conductor's resistance changes with temperature.
The DC resistance of a homogeneous conductor is proportional to its length and the material's resistivity, and inversely proportional to its cross-section: R = ρ·L/A. ρ is a temperature-dependent material constant, about 0.0175 Ω·mm²/m for copper at 20°C.
Much like a water pipe, greater length raises resistance and a larger cross-section lowers it. A long, thin extension cord behaves electrically like a long, narrow hose: at high current, a noticeable voltage drop develops along the cable length, just as a noticeable pressure loss develops along a hose at high flow.
R = ρ · L / A
R = ρ · L / AL = R · A / ρA = ρ · L / R| Symbol / input | Meaning |
|---|---|
| Conductor resistance R | Ohmic resistance at the stated temperature. |
| Resistivity ρ | Material property, e.g. copper about 0.0175 Ω·mm²/m at 20 °C. |
| Conductor length L | Electrical length; include both go and return conductors for voltage drop. |
| Conductor area A | Metal cross-section normal to current flow. |
Enter three of the four quantities to find the fourth. Use a ρ value matching the actual operating temperature, since many metals' resistivity changes with temperature. For voltage-drop calculations, L counts as the sum of the outgoing and return conductor.
Select the target quantity and enter the three known values with units. For a voltage-drop estimate, first calculate R and multiply by the expected operating current (Vdrop = R·I).
Given ρ = 0.0175 Ω·mm²/m (copper), L = 10 m and A = 10 mm², substitution gives R = 0.0175 · 10/10 = 0.0175 Ω.
A conductor resistance of 0.0175 Ω produces a voltage drop of about 0.28 V at, say, a 16 A operating current over this 10 m run. Doubling length or halving cross-section would quadruple or double that voltage drop respectively.
Resistivity is given in Ω·mm²/m (convenient for cross-sections in mm²) or Ω·m (SI-coherent). Conductor resistance is given in Ω, or mΩ for very thin or long conductors.
Copper's resistivity rises with a temperature coefficient of about 3.9×10⁻³ per °C, roughly 0.39% per kelvin. A copper conductor heated from 20°C to 70°C therefore has about 20% higher resistance than at 20°C. For cables that run noticeably hot in service — from heavy continuous load or unfavourable installation conditions — resistivity should be corrected to the actual operating temperature rather than using the uncorrected 20°C table value.
Conductor resistance calculations are used to size cable cross-sections for long cable runs, estimate voltage drop in extension cords and solar installations, and design windings for motors and transformers.
The formula applies to DC at constant temperature with a homogeneous cross-section. At high-frequency AC, the skin effect reduces the effectively used conductor cross-section and raises AC resistance above the DC value calculated here.
Common mistake: For voltage-drop calculations, don't forget that current flows through both the outgoing and return conductor — the relevant length is therefore double the one-way cable length if both are to be captured in the same formula. Also, don't take resistivity from a 20°C table uncorrected if the conductor runs noticeably hotter in operation.
Conductor resistance converts part of the electrical power to heat (P = I²·R). With too small a cross-section and high current, this heat generation can become excessive.
For copper, about 0.39% per kelvin. A conductor heated from 20°C to 70°C has about 20% more resistance than at 20°C.
Because current flows through both the outgoing and return conductor; both lengths add up to the relevant total resistance.