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Resistivity Calculator (R = ρL/A)

Resistance is not a property of a material on its own; it is a property of a particular piece of it. This calculator applies R = ρL/A so you can see why a long thin wire drops voltage and a short fat one does not.

Laws of Resistance — R = ρL/A

Resistance from the material's resistivity and the conductor's dimensions. Fill any three of R, ρ, L, A and leave the fourth blank. (Copper ρ ≈ 1.68 µΩ·m.)

Resistance R
Resistivity ρ
Length L
Cross-section A
Conductance G
  1. 1.Given three of four: R, ρ, L, A
  2. 2.FormulaR = ρ·L / ASubstituteR = 1.68e-6 × 100 ÷ 1e-6ResultR = 168 Ω
  3. 3.FormulaConductance G = 1 / RSubstituteG = 1 ÷ 168ResultG = 5.9524 mS
Common trap: Resistance is proportional to length but inversely to cross-section — a wire twice as thick (double the area) has half the resistance, not double. And for metals resistance rises with temperature (positive α); for semiconductors and carbon it falls.

The formula

R = ρ × L / A

R
resistance of the piece (ohms)
ρ
resistivity of the material (ohm·metres)
L
length along the current path (metres)
A
cross-sectional area (square metres)

Worked example

10 m of copper wire with a 1 mm² cross-section (ρ = 1.68 × 10⁻⁸ Ω·m).

  1. Convert the area: 1 mm² = 1 × 10⁻⁶ m²
  2. R = (1.68 × 10⁻⁸ × 10) / (1 × 10⁻⁶)
  3. R = 1.68 × 10⁻⁷ / 1 × 10⁻⁶

R = 0.168 Ω — small, but at 16 A that is already 2.7 V lost in the cable.

Where you'll use it

Cable sizing, shunt design, and the standard exam question about doubling a wire's length or halving its diameter. Also explains why resistors drift with temperature, since ρ itself is temperature-dependent.

The laws behind it

Parts this applies to

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