Electrical Conductance Calculator

Calculate electrical conductance, conductivity, and resistivity for conductors. Compare materials, wire gauges, and temperature effects on conduction.

Conductance (G)
1.4501 S
= 1/R = 1/0.6896 Ω
Resistance (R)
689.6000 mΩ
At 20°C
Conductivity (σ)
58.00 MS/m
100.0% IACS
Resistivity (ρ)
1.7240 µΩ·cm
1.7240 × 10⁻⁸ Ω·m
R per 100m
0.6896 Ω/100m
G per 100m = 1.4501 S
Temp Coefficient (α)
3.93 mΩ/Ω/°C
ΔR = 0.0% from 20°C

Material Conductivity (%IACS)

Silver
108%
Copper
100%
Gold
70.7%
Aluminum
61%
Tungsten
31%
Zinc
29%
Nickel
25%
Iron
17.6%

Power Loss at Various Currents

Current (A)Voltage Drop (V)Power Loss (W)
0.10.0690.007
0.50.3450.172
10.6900.690
53.44817.240
106.89668.960
2013.792275.840
5034.4801,724.000
10068.9606,896.000
Material Comparison (same geometry)
Material%IACSR (Ω)G (S)
Silver1080.63481.5753
Copper (annealed)1000.68961.4501
Gold70.70.97601.0246
Aluminum611.06000.9434
Tungsten312.24000.4464
Zinc292.36000.4237
Nickel252.79600.3577
Iron17.63.88400.2575
Brass262.52000.3968
Stainless Steel 3042.428.80000.0347
Nichrome1.544.00000.0227
Planning notes, formulas, and examples

About the Electrical Conductance Calculator

The Electrical Conductance Calculator computes conductance (G), conductivity (σ), and resistivity (ρ) for conductors of various materials and geometries. Conductance is the reciprocal of resistance — it measures how easily current flows through a material and is measured in siemens (S). That makes it a useful companion to resistance when you are comparing conductors by practical current flow. It is especially handy when you want to compare a conductor's performance without rewriting everything in terms of ohms. The same framework also makes it easier to compare wire sizes, materials, and temperature effects on a single page, especially when you are reviewing busbars, cable runs, or winding choices.

Conductance depends on the material's conductivity, the conductor's cross-sectional area, and its length. Copper, aluminum, silver, and gold are the most conductive metals. At the system level, conductance simplifies parallel circuit analysis — parallel conductances add directly, unlike resistances which require reciprocal addition.

Enter conductor dimensions and material properties to calculate conductance, resistance, and compare with other materials. The calculator includes a comprehensive materials database with %IACS conductivity ratings (International Annealed Copper Standard).

When This Page Helps

Use this calculator when you need to compare materials or wire sizes by how easily they carry current, not just by resistance alone. It is useful for conductor selection, temperature correction, and parallel-circuit analysis where conductance is the cleaner way to think about the problem. It also makes unit conversions between resistivity and conductivity less error-prone, which helps when you are comparing multiple conductors on the same basis.

How to Use the Inputs

  1. Select the conductor material from the dropdown.
  2. Enter the conductor length.
  3. Enter the cross-sectional area (or use wire gauge selection).
  4. Review conductance, resistance, and per-unit values.
  5. Optionally enter operating temperature for temperature correction.
  6. Compare conductance across materials in the reference table.
Formula used
Conductance: G = σ × A / L = 1/R (siemens). Conductivity: σ = 1/ρ (S/m). Resistance: R = ρ × L / A (ohms). Temperature Correction: ρ(T) = ρ₂₀ × [1 + α × (T - 20°C)]. Where ρ = resistivity (Ω·m), L = length (m), A = cross-section area (m²), α = temperature coefficient.

Example Calculation

Result: G = 1.45 S, R = 0.689 Ω

Copper ρ = 1.724×10⁻⁸ Ω·m. Area = 2.5 mm² = 2.5×10⁻⁶ m². R = 1.724×10⁻⁸ × 100 / 2.5×10⁻⁶ = 0.690 Ω. G = 1/R = 1.45 S.

Tips & Best Practices

  • For power transmission, aluminum is preferred over copper due to lower cost per unit conductance.
  • Stranded wire has slightly higher resistance than solid wire of the same gauge due to fill factor.
  • At high frequencies (>100 kHz), skin effect reduces the effective conductor area significantly.
  • Superconductors have infinite conductance (zero resistance) below their critical temperature.
  • Alloys generally have lower conductivity than pure metals — brass is only 26% IACS vs copper at 100%.

Material Conductivity Reference

Common conductor materials and their approximate conductivity at 20°C: Silver: 6.30×10⁷ S/m (108% IACS). Copper (annealed): 5.80×10⁷ S/m (100% IACS). Gold: 4.11×10⁷ S/m (70.7% IACS). Aluminum: 3.50×10⁷ S/m (61% IACS). Brass: 1.59×10⁷ S/m (26% IACS). Iron: 1.04×10⁷ S/m (17.6% IACS). Stainless Steel 304: 1.39×10⁶ S/m (2.4% IACS). Nichrome: 9.09×10⁵ S/m (1.5% IACS).

The vast range of conductivity — from 6×10⁷ for silver to 10⁻¹⁴ for glass — spans over 20 orders of magnitude, making it one of the widest-ranging physical properties.

Temperature Effects on Conductance

Metal conductance decreases with temperature because lattice vibrations scatter conduction electrons. The linear approximation G(T) = G₂₀ / [1 + α(T-20)] works well from -50°C to +200°C. Temperature coefficients: copper α = 0.00393/°C, aluminum α = 0.00429/°C, iron α = 0.00651/°C. Note that semiconductors show the opposite behavior — their conductance increases with temperature as more electrons gain enough energy to enter the conduction band.

Applications in Circuit Analysis

Conductance simplifies many circuit problems. In nodal analysis, the conductance matrix (G matrix) is symmetric positive definite, making it computationally efficient. Power dissipation through a conductance: P = V²G = I²/G. Thermal conductance (watts per kelvin) is analogous — Fourier's law of heat conduction has the same mathematical form as Ohm's law.

Sources & Methodology

Last updated:

Frequently Asked Questions

  • Conductivity (σ, measured in S/m) is a material property — it doesn't change with size or shape. Conductance (G, measured in siemens) depends on both the material and geometry (area and length). Conductance = Conductivity × Area / Length. That is why a short thick wire can conduct much better than a long thin one of the same material.