Magnetostatics & the Biot-Savart Law
Steady currents create static magnetic fields. The Biot-Savart law gives the field from any current distribution; for symmetric geometries, Ampere's law (the magnetic analog of Gauss's law) is far more efficient. The divergence of B is always zero — there are no magnetic monopoles.
Key Concepts
Key Equations
Field of a Long Straight Wire
A long straight wire carries A. Find at m from the wire.
By symmetry, use Ampere's law with a circular loop of radius :
Exercises
7 problemsA long wire carries A. Find at m (in μT). , T·m/A.
A solenoid has turns/m and A. Find inside (in mT).
A circular loop (radius m) carries A. Find at the center (in μT). .
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Upgrade to Pro →Force per unit length between two parallel wires 0.30 m apart, each carrying A in the same direction (in N/m). Attractive or repulsive? .
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Upgrade to Pro →A toroid has turns, mean radius m, and A. Find inside (in mT). .
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Upgrade to Pro →A magnetic dipole has A·m². Find the torque (in N·m) in a uniform T field at ().
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Upgrade to Pro →A proton ( C, kg) enters a T field perpendicular to it at m/s. Find the cyclotron radius (in cm).
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Upgrade to Pro →Key Takeaways
- Biot-Savart law gives from any current; Ampere's law is efficient for symmetric configurations.
- Infinite wire: . Solenoid: (uniform inside, zero outside).
- always — no magnetic monopoles. enforces this.
- Parallel currents attract; anti-parallel repel. This defines the SI ampere.