Theme D · Fields
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Theme D · Fields

Chapter 2 · HL induction

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Magnetic flux
Φ=BAcosθ\Phi = BA\cos\theta
Webers (Wb); max when field ⟂ surface.
Faraday's law
ε=NdΦdt\varepsilon = -N\frac{d\Phi}{dt}
EMF = rate of change of flux linkage.
Lenz's law (the minus sign)
Induced current opposes the change that made it — energy conservation.
No change → no EMF
A stationary magnet in a coil induces nothing; flux must be *changing*.
Motional EMF (rod)
ε=BvL\varepsilon = BvL
Rod length LL moving at vv across field BB.
Transformer
VsVp=NsNp\frac{V_s}{V_p} = \frac{N_s}{N_p}
Step up/down AC voltage via turns ratio.
Ideal transformer power
VpIp=VsIsV_pI_p = V_sI_s
Step UP voltage ⇒ step DOWN current (power conserved if 100% efficient).
Flux linkage
NΦN\Phi
Units Wb (= T m²); the bigger this changes per second, the bigger the EMF.
Motor effect (the reverse)
F=BILF = BIL
Current in a field feels a force; reverse current OR field to reverse it.
Key SI units
Φ\Phi: Wb · BB: T · AA: m² · ε,V\varepsilon, V: V · NN: (no unit) · dΦdt\tfrac{d\Phi}{dt}: Wb s⁻¹ = V.
Common traps
Dropping the minus sign / forgetting Lenz; a steady (unchanging) flux gives ZERO EMF; using θ\theta from the surface instead of the normal in Φ=BAcosθ\Phi=BA\cos\theta.