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Biot–Savart law

Intermediate

Field from a current element.

Key relationdB = μ₀Idl×r̂/4πr²

The field from a current element: dB = (μ₀/4π) I dl × r̂/r². Integrating gives fields of wires, loops and coils.

Worked example

Field of a loop at the centre: μ₀I/2R.

Common mistake

Direction: right-hand rule.

In more detail

The Biot-Savart law gives the magnetic field produced by a small current element, dB = (μ0/4π) I dl × r̂ / r². It is the magnetic analogue of Coulomb's law for a current source.

Real-world uses

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Frequently asked questions

Is it the same as Coulomb's law?

Similar in form, but it uses a cross product because the field is perpendicular to the current element.

Why is it integrated?

Because a current distribution is made of many small elements, whose fields add.

Is the Biot–Savart law the same as Ampere's law?

They are equivalent for steady currents, but Biot–Savart is easier for finding the field of a finite current element.

Related topics in Magnetism & Induction

Torque on a current loop · Moving coil galvanometer · Electric motor · Field of a long straight wire · Field at centre of a loop · Field on axis of a coil

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