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Hall Coefficient Calculator (R_H = 1/nq, carrier density from Hall voltage)

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Understanding the Hall coefficient calculator — concept and principle

This calculator relates the Hall coefficient, the charge-carrier density and the Hall voltage of a conducting strip in a magnetic field. Give it the carrier density to predict the Hall voltage, or a measured Hall voltage to find the density. It is used in solid-state physics labs and to characterise semiconductors and metals.

Hall effect in copperHall voltage in a copper stripn8.34 × 10²⁸ m⁻³I · B10 A · 1 TThickness0.1 mmR_H = −1 ÷ (n e)V_H = I B ÷ (n e t)Hall coefficient−7.484 × 10⁻¹¹Hall voltage7.484 µVCarrierselectrons (−)R_H in m³/C
Copper has so many free electrons that even 10 A in 1 T gives only microvolts; the minus sign marks electrons.

How it is calculated

R_H = 1 ÷ (n q), negative for electrons and positive for holes

V_H = I B ÷ (n e t)

From a measured voltage: |R_H| = V_H t ÷ (I B) and n = 1 ÷ (|R_H| e)

The principle

Carriers drifting along a strip in a magnetic field feel a sideways magnetic force. They pile up on one edge until the electric field from that charge balances the magnetic force, and the voltage across the strip at that point is the Hall voltage. Fewer carriers must drift faster to carry the same current, so they feel a stronger force and produce a larger voltage; that is why V_H is inversely proportional to n. The sign of the voltage reveals whether the carriers are negative electrons or positive holes.

Worked example

Default inputs: from carrier density, electrons, n = 8.34 × 10²⁸ m⁻³, I = 10 A, B = 1 T, t = 0.1 mm.

  1. R_H = −1 ÷ (8.34 × 10²⁸ × 1.602 × 10⁻¹⁹) = −7.484 × 10⁻¹¹ m³/C.
  2. V_H = 10 × 1 ÷ (8.34 × 10²⁸ × 1.602 × 10⁻¹⁹ × 1 × 10⁻⁴) = 7.484 µV.
  3. Carrier density = 8.34 × 10²⁸ per m³; sign of the carriers: negative (electrons).

How to read the result

Metals have huge carrier densities, so their Hall voltages are only microvolts even with large currents and strong fields. Lightly doped semiconductors have far fewer carriers and give much larger voltages, which is why Hall sensors are made from semiconductors. A positive R_H shows that holes dominate.

Common mistakes

Keep in mind: The single-carrier model fits simple metals and strongly doped semiconductors. Mixed conduction needs a two-band analysis.

Frequently asked questions

Why is the Hall voltage so small in copper?

Copper has about 10²⁹ free electrons per cubic metre, so they drift slowly and the sideways force is small.

What does a positive Hall coefficient mean?

The current is carried mainly by positive holes, as in p-type semiconductors.

How is the Hall effect used in practice?

Hall sensors measure magnetic fields and detect position, speed and current without contact.

Sources: OpenStax, University Physics Volume 2 (2016), section 11.6 "The Hall Effect"

Checked 9 Nov 2026. OpenStax, University Physics Volume 2 (2016), §11.6 “The Hall Effect”: vd = E/B (Eq. 11.25), I = nevdA (Eq. 11.26), V = IBl/(neA) (Eq. 11.29), sign of V gives the sign of the carriers. RH = 1/(nq) — standard definition; e exact (2019 SI).

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