INGENIA

EMG-04

Faraday motional emf

ε = B ℓ v for a rod sliding on rails.

Reading speed
InductionFaraday 1831

Governing equation

E=Bℓv=−dΦBdt\mathcal{E}=B\ell v=-\dfrac{\mathrm{d}\Phi_B}{\mathrm{d}t}

v∈[0.05,20]v \in \left[0.05, 20\right]

where

B
Field (T)
\ell
Rod length (m)
v
Speed (m/s)
\mathcal{E}
Induced emf (V)

The figure, part by part

Each numbered marker wears the color of its card. Hover a card to light the marker. Tap a marker to jump to that card. The slider walks a red point along the curve; Animate drawing traces it like a pen.

EMG-04 · circuit
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①

Governing law — red

E=Bℓv=−dΦBdt\mathcal{E}=B\ell v=-\dfrac{\mathrm{d}\Phi_B}{\mathrm{d}t}

v∈[0.05,20]v \in \left[0.05, 20\right]

v=0.05v = 0.05E=0.006\mathcal{E} = 0.006

②

Domain of the variable — blue

vmin⁡=0.05,vmax⁡=20v_{\min} = 0.05,\quad v_{\max} = 20

v∈[0.05,20]v \in \left[0.05, 20\right]

v=0.05v = 0.05v=0.05v = 0.05

③

Response curve — green

E=Bℓv=−dΦBdt\mathcal{E}=B\ell v=-\dfrac{\mathrm{d}\Phi_B}{\mathrm{d}t}

v∈[0.05,20]v \in \left[0.05, 20\right]

v=0.05v = 0.05E=0.006\mathcal{E} = 0.006

④

Rate of change — amber

dEdv\frac{\mathrm{d}\mathcal{E}}{\mathrm{d}v}

v∈[0.05,20]v \in \left[0.05, 20\right]

v=0.175v = 0.175E′=0.12\mathcal{E}^{\prime} = 0.12

Lecture brief

Historical brief

Coulomb, Gauss, Ampère, Faraday and Maxwell (1861–65) unified charge, current and light. The lab computes fields, induction, Poynting flux and the electromagnetic wave in SI. This sheet (EMG-04 — Faraday motional emf) is the form associated with Faraday 1831. Working symbols: BB, ℓ\ell, vv →\rightarrow E\mathcal{E}. Faraday's law ε = −dΦB/dt for a changing area ℓ x(t) in a uniform B reduces to B ℓ v.

Purpose

Purpose: compute E\mathcal{E} from BB, ℓ\ell, vv in Electromagnetism via E=Bℓv=−dΦBdt\mathcal{E}=B\ell v=-\dfrac{\mathrm{d}\Phi_B}{\mathrm{d}t} ε = B ℓ v for a rod sliding on rails. Use it when a real electromagnetism question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given B=0.400 TB = 0.400\,\mathrm{T}, ℓ=0.300 m\ell = 0.300\,\mathrm{m}, v=2.000 m/sv = 2.000\,\mathrm{m/s}, the governing relation E=Bℓv=−dΦBdt\mathcal{E}=B\ell v=-\dfrac{\mathrm{d}\Phi_B}{\mathrm{d}t} yields E=0.2400 V\mathcal{E} = 0.2400\,\mathrm{V}. Uniform B perpendicular to the loop, constant v. Move a slider: the numbers are this situation, not a canned story.

Calculator

Inputs

Outputs

  • Induced emf \mathcal{E}0.2400 V
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EMG-04 · circuit
00:0 / 00:08

Narration of this film

Uniform B perpendicular to the loop, constant v.

Faraday's law ε = −dΦB/dt for a changing area ℓ x(t) in a uniform B reduces to B ℓ v.

Reading speed

Watch on YouTube