πŸ”¬ Beyond the Loop β€” Flux in Motion

Faraday’s law does not need a magnet or a textbook loop. See induction driven by a current-carrying wire, and by a single moving charge.
Every tab here is the same underlying law: emf = βˆ’NΒ·dΞ¦/dt. What differs each time is WHICH factor in Ξ¦ = NΒ·BΒ·AΒ·cosΞΈ is doing the changing β€” B, A, ΞΈ, or N itself.
What is this?
Apparatus β€” drag the highlighted parts
Flux Ξ¦ through the circuit β€” is it changing?
Induced EMF β€” Lenz's law in action
Which way does the current actually flow?
Live calculation