Magnetic force on charges and current elements, current-density definitions, and magnetic-field geometry; later chapters cover Biot–Savart and Ampère.
Magnetic field & magnetostatics
Magnetic force first fixes what a magnetic field does; stationary currents then supply source laws for calculating that field. We progress from moving charges through Biot–Savart and Ampère to vector potential, inductance and magnetic energy, without confusing steady-source assumptions with arbitrary time dependence.
- EM-01: electric field and potential
- Vector cross product and Newtonian motion
- Vector calculus basics and SI units
- Calculate force on moving charges and current elements.
- Compute B via Biot–Savart and Ampère with justified symmetry.
- Introduce vector potential without confusing gauge and field.
- Derive inductance and magnetic-energy balances.
Magnetic field & magnetostatics
Magnetic force first fixes what a magnetic field does; stationary currents then supply source laws for calculating that field. We progress from moving charges through Biot–Savart and Ampère to vector potential, inductance and magnetic energy, without confusing steady-source assumptions with arbitrary time dependence.
- 01→
Lorentz force
Define the operational electric and magnetic force on a moving point charge, derive the cross-product geometry, prove that a static magnetic field does no mechanical work, solve constant-B circular/helical motion and carry the result to the force on a current element. Distinguish a force law for given fields from source laws for computing those fields.
220–280 min · Intermediate → advanced · available - 02→
Biot–Savart law
Compute magnetostatic B from a prescribed steady current: derive and interpret the filament and current-density integrals, identify source/observation coordinates and right-hand orientation, and integrate the finite and infinite straight wire and the on-axis circular loop. Distinguish the source law from the Lorentz force, specify steady divergence-free currents and the thin-filament idealization, and check signs, dimensions, limits and singular endpoints.
250–310 min · Intermediate → advanced · available - 03→
Ampère's law
From the magnetostatic curl equation to the integral circulation law, distinguish current enclosed from the local field on a chosen loop. Derive straight-wire, uniformly filled cylindrical conductor and ideal infinite current-sheet fields using actual symmetries; demonstrate why zero circulation or zero enclosed current is not a local zero-field criterion; identify the time-varying displacement-current correction.
240–300 min · Intermediate → advanced · available - 04→
Magnetic vector potential
Construct B as the curl of a vector potential and distinguish gauge freedom from physical magnetic flux. Under a declared stationary localized-current/Coulomb-gauge model, derive the vector Poisson equation and its Green-kernel solution, recover Biot–Savart by taking a curl, compare symmetric and Landau gauges for uniform B, and explain why infinite-wire potentials require a finite reference radius.
250–310 min · Advanced · available - 05→
Inductance and magnetic energy
Define oriented magnetic flux linkage and self/mutual inductance; derive reversible U=∫I dλ and ½LI² for fixed linear geometry, compute an ideal long-solenoid inductance and field-energy cross-check, obtain a rectangular-cross-section toroid's logarithmic result, and distinguish reciprocity, passivity, loss, nonlinear magnetic media and dispersion.
270–330 min · Advanced · available
References
Core field texts are combined with SI units and explicit nonrelativistic limits.
Operational force laws, vector cross products and relative-motion context.
Classical magnetostatic source laws, field derivations and the limits of static approximations.
SI definitions and consistent use of the tesla, newton, ampere, coulomb and volt.