Formulas and conditions only — no derivations, no solved numbers. The diagrams are the reader's own.
I
Displacement current
FLUX CHANGING, NOT CHARGE MOVING
I.DefinitionID = ε0dΦEdtnothing crosses the gap
II.Ampère–Maxwell∮ B·dl = μ0 (I + ID)
III.In a charging capacitorID = Iby identity, not by conduction
IV.Gauss, electric∮ E·dA = qε0
V.Gauss, magnetic∮ B·dA = 0no monopoles
VI.Faraday∮ E·dl = − dΦBdt
The displacement current exists to keep Ampère's law consistent whichever surface you stretch across the loop. Maxwell added it on paper; the wave it predicted arrived twenty years later.
II
The wave itself
E AND B PEAK TOGETHER
I.Speed in vacuumc = 1√(μ0 ε0)3.00×108 m s−1
II.In a mediumv = cn , n = √(μr εr)
III.Field ratioE0B0 = c
IV.GeometryE ⊥ B ⊥ direction of traveltransverse, and in phase
V.Frequency in a mediumunchangedλ and v both drop by n
VI.Energy densityu = 12 ε0 E² + B²2μ0the two halves are equal