Magnetism and Electromagnetic Induction Cheat Sheet
The core ideas of Magnetism and Electromagnetic Induction distilled into a single, scannable reference — perfect for review or quick lookup.
Quick Reference
Magnetic Force on a Moving Charge
A charge $q$ moving with velocity $\vec{v}$ in a magnetic field $\vec{B}$ experiences a force $\vec{F} = q\vec{v} \times \vec{B}$. The magnitude is $F = qvB\sin\theta$, where $\theta$ is the angle between $\vec{v}$ and $\vec{B}$. The force is always perpendicular to both $\vec{v}$ and $\vec{B}$, so it changes direction but not speed.
Magnetic Force on a Current-Carrying Wire
A straight wire of length $L$ carrying current $I$ in a magnetic field $\vec{B}$ experiences a force $\vec{F} = I\vec{L} \times \vec{B}$, with magnitude $F = BIL\sin\theta$. This force is the basis for electric motors, where current loops rotate in magnetic fields to produce mechanical work.
Magnetic Field from a Long Straight Wire
A long straight wire carrying current $I$ produces a magnetic field that circles the wire concentrically: $B = \mu_0 I / (2\pi r)$, where $\mu_0 = 4\pi \times 10^{-7}$ T m/A is the permeability of free space and $r$ is the distance from the wire. The direction follows the right-hand rule.
Solenoid and Its Magnetic Field
A solenoid is a coil of wire wound in a helix. Inside a long solenoid, the field is nearly uniform: $B = \mu_0 n I$, where $n$ is the number of turns per unit length and $I$ is the current. The field outside is approximately zero. Solenoids are used in electromagnets, relays, and MRI machines.
Ampere's Law
The line integral of the magnetic field around any closed loop equals $\mu_0$ times the enclosed current: $\oint \vec{B} \cdot d\vec{l} = \mu_0 I_{\text{enc}}$. This is the magnetic analog of Gauss's law and is most useful for calculating fields with high symmetry (infinite wires, solenoids, toroids).
Magnetic Flux
The magnetic flux through a surface is $\Phi_B = \int \vec{B} \cdot d\vec{A}$. For a uniform field through a flat loop: $\Phi_B = BA\cos\theta$, where $\theta$ is the angle between $\vec{B}$ and the surface normal. The SI unit is the weber (Wb = T m$^2$).
Faraday's Law of Induction
A changing magnetic flux through a loop induces an EMF: $\varepsilon = -N \, d\Phi_B/dt$, where $N$ is the number of turns. The EMF drives a current if the loop is part of a complete circuit. This is the operating principle of generators, transformers, and many sensors.
Lenz's Law
The direction of an induced current is always such that it opposes the change in magnetic flux that produced it. This is a consequence of conservation of energy: if the induced current aided the flux change, it would create a perpetual motion machine. The negative sign in Faraday's law encodes Lenz's law.
Electromagnetic Waves
Self-propagating oscillations of perpendicular electric and magnetic fields that travel at the speed of light: $c = 1/\sqrt{\mu_0 \epsilon_0} \approx 3 \times 10^8$ m/s. Predicted by Maxwell's equations, they span the spectrum from radio waves to gamma rays and require no medium for propagation.
Key Terms at a Glance
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