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12.4 Ampère’s 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.

Ampère’s Law is the magnetic analogue of Gauss’s law for highly symmetric current distributions. It states

∮B⋅dℓ=μ0Ienc\oint \mathbf{B} \cdot d\mathbf{\ell} = \mu_0 I_{\text{enc}}

This means the circulation of the magnetic field around a closed loop equals μ0{\mu_0} times the net current enclosed by the loop. Ampère’s law is most useful when symmetry allows B to be constant in magnitude along parts of the loop and parallel to dℓ{d\mathbf{\ell}}.

For a long straight wire, choosing a circular Amperian loop gives

B(2πr)=μ0IB(2\pi r) = \mu_0 I

so

B=μ0I2πrB = \frac{\mu_0 I}{2\pi r}

For an ideal solenoid, Ampère’s law gives

B=μ0nIB = \mu_0 n I

inside, where n is turns per unit length, and approximately zero outside. For a toroid, the field is

B=μ0NI2πrB = \frac{\mu_0 N I}{2\pi r}

inside the core region. Ampère’s law is therefore the fastest route to magnetic fields in systems with cylindrical or loop symmetry.

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