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12.3 Magnetic Fields of Current-Carrying Wires and the Biot-Savart Law

Part of Magnetic Fields and Electromagnetism in AP® Physics C: Electricity and Magnetism. Read the opening section, then create a free account for the full interactive lesson, practice, and progress tracking.

A current produces a magnetic field. For a small current element, the field contribution is described by the Biot-Savart Law:

dB=μ04πI dℓ×r^r2d\mathbf{B} = \frac{\mu_0}{4\pi}\frac{I \, d\mathbf{\ell} \times \hat{\mathbf{r}}}{r^2}

This means the magnetic field depends on the current, the geometry of the wire, the location of the observation point, and the inverse square of the distance from the current element. The direction is determined by the cross product, which is why the magnetic field wraps around a straight wire in circular loops.

For highly symmetric cases, the Biot-Savart integral leads to standard results. For a long straight wire,

B=μ0I2πrB = \frac{\mu_0 I}{2\pi r}

and for the center of a circular loop of radius R,

B=μ0I2RB = \frac{\mu_0 I}{2R}

for one loop. The Biot-Savart law is powerful because it builds magnetic fields from source currents directly, but it is most practical when the geometry is simple or highly symmetric.

In this unit

4 lessons

  1. 12.1Magnetic FieldsPreview lesson
  2. 12.2Magnetism and Moving ChargesPreview lesson
  3. 12.3Magnetic Fields of Current-Carrying Wires and the Biot-Savart LawThis lesson
  4. 12.4Ampère’s LawPreview lesson

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