MAGNETISM & ELECTROMAGNETISM SIMULATION

Cut a bar magnet in half and you never get a loose north pole and a loose south pole, only two smaller magnets that each have both. The reason lies inside: the material is divided into countless magnetic domains, and the stronger the applied field the more of them rotate into alignment, while heating past the Curie point scrambles them again and the bar loses its magnetism. Faraday supplied the remaining crucial point: a magnet sitting still inside a coil leaves the meter needle at zero, since only a changing flux can generate an EMF.

▸ Building magnet & magnetic field lines N→S…
▸ Feeding current → generating magnetic field (Oersted)
▸ Loading electromagnetic induction (Faraday) e = −dΦ/dt
▸ Mounting the coil — motor & generator
▸ Ready — Online. ✅
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Simulation room Magnetism & Electromagnetism

Magnetism & Electromagnetism
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electricity ⇄ magnetism
Electromagnetic meter
🧲 B · I · EMF · rotations
Induced EMF ∝ rate of change of magnetic flux
Magnetic field B—
Current I—
EMF—
Rotation speed—
Scenario—
Viewing—
Notes
Current creates a magnetic field (Oersted); a changing field induces a current (Faraday). The force F=B·I·L turns the coil → motor; spinning the coil → generator.
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Induced current & EMF over time current IEMF
About Electromagnetism

Cut a bar magnet in half and you never get a loose north pole and a loose south pole, only two smaller magnets that each have both. The reason lies inside: the material is divided into countless magnetic domains, and the stronger the applied field the more of them rotate into alignment, while heating past the Curie point scrambles them again and the bar loses its magnetism. Faraday supplied the remaining crucial point: a magnet sitting still inside a coil leaves the meter needle at zero, since only a changing flux can generate an EMF.

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