Conductivity to Resistivity Calculator

Conductivity ↔ Resistivity Converter

Convert between electrical conductivity and resistivity for material characterization and electrical engineering applications.

Materials Science • Electrical Engineering • 2024

Calculation

Resistivity ρ (Ω·m)

1.6779e-8

Formula: ρ = 1 / σ

Conductivity vs Resistivity

Electrical conductivity σ (siemens per meter, S/m) measures material's ability to conduct electric current. Resistivity ρ (ohm-meters, Ω·m) measures material's opposition to current. Relationship: ρ = 1/σ (reciprocal). Perfect reciprocal relationship means doubling conductivity halves resistivity. Conductivity units: S/m = 1/(Ω·m). Higher conductivity → easier electron flow → lower resistivity. Examples: Copper (excellent conductor) σ ≈ 5.96×10⁷ S/m → ρ ≈ 1.68×10⁻⁸ Ω·m (extremely low resistivity). Air (insulator) σ ≈ 10⁻¹⁵ S/m → ρ ≈ 10¹⁵ Ω·m (huge resistivity). Semiconductors (intermediate) silicon σ ≈ 10⁻⁶ S/m → ρ ≈ 10⁶ Ω·m. Temperature dependence: metals conductivity decreases with temperature (increased atomic vibration scatters electrons); semiconductors increase with temperature (more mobile charge carriers). Hall coefficient extends this: combines conductivity with magnetic field measurements to determine charge carrier type (electrons vs holes) and concentration. Practical engineering: wire gauge selection based on resistivity; higher resistivity requires larger diameter to achieve target resistance.

Material science applications: conductivity measurements characterize material purity (impurities increase conductivity sometimes or decrease, depending on dopant type in semiconductors). Anisotropic materials: single crystals exhibit directional dependence—different conductivity along different crystal axes. Tensor representation: σ_ij for general case. Superconductivity: perfect conductor achieved at low temperature—σ → ∞, ρ → 0 (zero resistance). Frequency-dependent effects: conductivity changes with signal frequency (AC vs DC); skin effect causes current concentration near surface in conductors. Ionic conductivity in electrolytes: ions carry current instead of electrons; formula ρ = 1/σ still applies. Temperature coefficient: α = (1/ρ₀)(dρ/dT); metals positive (resistivity increases), semiconductors negative (resistivity decreases). Contact resistance: material interfaces have additional resistance beyond bulk resistivity; important in integrated circuits. Grounding and shielding: low-resistivity materials preferred for current paths; high-conductivity metals (copper, aluminum) used for EMI shielding.

How to Convert

1

Know Measured Conductivity: Measure or look up σ in S/m (siemens per meter).

2

Check Units: Ensure conductivity in S/m (not μS/cm or other units).

3

Apply Reciprocal: ρ = 1/σ. Simple inversion formula.

4

Result in Ω·m: Resistivity automatically in ohm-meters.

5

Convert if Needed: To Ω·cm: multiply by 100. To MΩ·cm: divide by 10⁶.

Example: Common Materials

Material Comparison Table (at 20°C):

Materialσ (S/m)ρ (Ω·m)
Silver6.30×10⁷1.59×10⁻⁸
Copper5.96×10⁷1.68×10⁻⁸
Aluminum3.50×10⁷2.86×10⁻⁸
Tungsten1.89×10⁷5.28×10⁻⁸
Silicon10⁻⁶10⁶
Glass10⁻¹¹10¹¹

Copper example: σ = 5.96×10⁷ S/m → ρ = 1/(5.96×10⁷) = 1.68×10⁻⁸ Ω·m. Perfect reciprocal.

Frequently Asked Questions

Why are conductivity and resistivity reciprocals?

Fundamental physics: current flow opposed by material structure. Inverse relationship emerges from Ohm's law; no true exception known.

Which is more useful in practice?

Conductivity for materials science (measure of electron mobility). Resistivity for circuit design (calculate wire losses). Choose based on context.

How does temperature affect these?

Metals: conductivity decreases with T (atomic vibrations scatter electrons). Semiconductors: conductivity increases with T (more mobile charge carriers).

What units should I use?

SI units: σ in S/m, ρ in Ω·m. Older units: σ in mho/cm, ρ in Ω·cm. 1 S/m = 10 mho/cm. Always specify units.

Can conductivity be zero?

Theoretically never (infinite resistance). Practical insulators have σ ~10⁻¹⁸ S/m (nearly infinite ρ). Perfect insulators don't exist in practice.

How does doping affect semiconductors?

Adding impurities increases conductivity dramatically (millions of times). p-doping (holes) and n-doping (electrons) fine-tune conductivity.

What's superconductivity?

State where σ → ∞, ρ → 0 (perfect conductor) below critical temperature. Electrons pair (Cooper pairs), zero resistance flow.

Why do alloys have different conductivity?

Crystalline defects, atomic disorder increase scattering. Alloys less conductive than pure metals. Brass (Cu+Zn) less conductive than pure copper.

Conductivity-resistivity conversions are essential for material selection, electrical design, semiconductor engineering, and characterizing conducting properties of materials.

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