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electromagnetic field as a unified model

Learning objectives

  • Outcome

    State the two reciprocal relations — a changing magnetic field produces an electric field (Faraday's law) and a changing electric field produces a magnetic field (displacement current) — and identify which one follows from Faraday's law.

  • Outcome

    Distinguish E⃗\vec{E} and B⃗\vec{B} as two aspects of a single electromagnetic field: for a static charge, a steady current, and an electromagnetic wave, state which field components are non-zero.

  • Outcome

    Calculate the wave speed from c=1/μ0ε0c=1/\sqrt{\mu_0\varepsilon_0} and compare the result with the tabulated speed of light, estimating the relative deviation.

  • Outcome

    Sketch a plane electromagnetic wave and label the mutually perpendicular E⃗\vec{E}, B⃗\vec{B}, and the direction of propagation.

Understand the idea

The electromagnetic field as a unified model

Text

Before Maxwell, electric and magnetic phenomena were described by separate laws. Faraday's experiments showed that a changing magnetic flux creates a circulating electric field, so a changing B⃗\vec{B} produces an E⃗\vec{E}. Maxwell added the symmetric statement: a changing electric field is equivalent to a displacement current Id=ε0 dΦE/dtI_d=\varepsilon_0\,d\Phi_E/dt and itself produces a magnetic field. Therefore E⃗\vec{E} and B⃗\vec{B} cannot be treated separately: they are two aspects of one electromagnetic field, and this mutual generation makes a free wave possible without any charges or currents. In vacuum such a wave travels at c=1/μ0ε0≈3,00×108c=1/\sqrt{\mu_0\varepsilon_0}\approx 3{,}00\times10^{8} m/s, which matched the measured speed of light and became the main argument for the unified model. In this model E⃗\vec{E} and B⃗\vec{B} turn into each other when you change inertial frame, so the split into “electric” and “magnetic” depends on the observer.

Worked examples

Direct

Problem

Estimate the speed of an electromagnetic wave in vacuum from c=1/μ0ε0c=1/\sqrt{\mu_0\varepsilon_0}, taking μ0=4π×10−7\mu_0=4\pi\times10^{-7} H/m and ε0=8.85×10−12\varepsilon_0=8.85\times10^{-12} F/m. Compare the result with the tabulated value c=2.998×108c=2.998\times10^{8} m/s.

Solution

Step 1. Multiply the constants:

μ0ε0=(4π×10−7)(8.85×10−12)≈1.11×10−17 s2/m2.\mu_0\varepsilon_0=(4\pi\times10^{-7})(8.85\times10^{-12})\approx 1.11\times10^{-17}\ \text{s}^2/\text{m}^2.

Step 2. Take the reciprocal square root:

c=11.11×10−17=13.33×10−9≈3.00×108 m/s.c=\frac{1}{\sqrt{1.11\times10^{-17}}}=\frac{1}{3.33\times10^{-9}}\approx 3.00\times10^{8}\ \text{m/s}.

Step 3. Relative deviation:

3.00−2.9982.998≈0.07 %.\frac{3.00-2.998}{2.998}\approx 0.07\ \%.

The agreement with the tabulated value shows that light is an electromagnetic wave, and that E⃗\vec{E} and B⃗\vec{B} describe one field: the speed cc is fixed by the properties of vacuum alone.

Application

Problem

A plane electromagnetic wave travels along the zz axis in vacuum with Ex=E0sin⁡(kz−ωt)E_x=E_0\sin(kz-\omega t), where E0=300E_0=300 V/m. Find the amplitude and direction of the magnetic field of the wave and explain why such a wave does not die out in empty space.

Solution

Direction. In the unified model B⃗\vec{B} is perpendicular both to E⃗\vec{E} and to the direction of propagation, so By≠0B_y\ne 0 while Bx=Bz=0B_x=B_z=0. The triple E⃗\vec{E}, B⃗\vec{B}, v⃗\vec{v} is right-handed: E⃗×B⃗\vec{E}\times\vec{B} points along +z+z.

Amplitude. For a wave in vacuum E/B=cE/B=c, hence

B0=E0c=3003.00×108=1.0×10−6 T.B_0=\frac{E_0}{c}=\frac{300}{3.00\times10^{8}}=1.0\times10^{-6}\ \text{T}.

Why the wave does not die out. A changing electric field creates a magnetic field, and a changing magnetic field creates an electric field again. The field sustains itself and carries energy away from the source; charges and currents are needed only to emit the wave, not to keep it travelling.

Transfer

Problem

A circular capacitor of radius R=5.0R=5.0 cm is being charged by a current I=2.0I=2.0 A. Assuming the field between the plates is uniform, find the magnetic field at a distance r=R/2r=R/2 from the axis and at the edge of the plates r=Rr=R, where outside the field is given by Ampère's law for a wire carrying current II. Explain what the unified field model demonstrates here.

Solution

Between the plates the magnetic field is produced not by a conduction current but by a displacement current. With uniform charging, the share of displacement current inside radius rr is I r2/R2I\,r^2/R^2, so Ampère's law gives

B⋅2πr=μ0Ir2R2 ⇒ B=μ0Ir2πR2.B\cdot 2\pi r=\mu_0 I\frac{r^2}{R^2}\ \Rightarrow\ B=\frac{\mu_0 I r}{2\pi R^2}.

At r=R/2r=R/2:

B=4π×10−7⋅2.0⋅0.0252π⋅(0.050)2=4.0×10−6 T.B=\frac{4\pi\times10^{-7}\cdot 2.0\cdot 0.025}{2\pi\cdot(0.050)^2}=4.0\times10^{-6}\ \text{T}.

At the edge of the plates the same formula gives

B=μ0I2πR=4π×10−7⋅2.02π⋅0.050=8.0×10−6 T.B=\frac{\mu_0 I}{2\pi R}=\frac{4\pi\times10^{-7}\cdot 2.0}{2\pi\cdot 0.050}=8.0\times10^{-6}\ \text{T}.

What this demonstrates. Outside the capacitor the field equals that of a wire carrying current II, while inside it is produced by the changing electric field. The field is continuous at the edge and never “switches” from one origin to another: it is a single electromagnetic field, for which conduction current and displacement current are two interchangeable sources.

Practice

Text

Self-check with a simulation (safe, no equipment). Open a single-charge simulation, for example PhET “Radio Waves & Electromagnetic Fields”.

  1. Place the charge at rest. Note what you see: only E⃗\vec{E}, no magnetic field.
  2. Make the charge oscillate. Describe what appears around it: what the E⃗\vec{E} and B⃗\vec{B} lines look like and where the wave travels.
  3. Estimate from the picture the angle between E⃗\vec{E} and B⃗\vec{B} and between each of them and the direction of propagation; check that they are perpendicular.
  4. Double the oscillation frequency and note how the wavelength changes; compare with λ=c/f\lambda=c/f.
  5. Write a one-sentence conclusion: why the field far from the charge keeps existing.

Optional (safe). Build a circuit from a 1.5 V cell, a piece of insulated wire, and a compass: when you close the circuit for 2–3 s the needle deflects. Use battery power only, never mains; the wire may warm up, so open the circuit immediately.

Visual reference

Purpose

Show that the electric and magnetic fields are not two independent objects but two mutually perpendicular components of one travelling wave that sustain each other.

Representation

An axonometric sketch: the zz axis is the direction of propagation; a sine curve for E⃗\vec{E} in the xzxz plane with amplitude E0E_0; a sine curve for B⃗\vec{B} in the yzyz plane with amplitude B0=E0/cB_0=E_0/c; the arrows E⃗\vec{E}, B⃗\vec{B}, and v⃗\vec{v} are mutually perpendicular; labels “E/B=cE/B=c” and one wavelength λ\lambda between two neighbouring maxima.

Real-world examples

Mobile communication and Wi‑Fi: a radio wave as a unified electromagnetic field

Scenario

A phone lies 3 m3\ \text{m} from a Wi‑Fi router transmitting at 2.4 GHz2.4\ \text{GHz}. The router's antenna current oscillates 2.4×1092.4\times10^9 times per second, so one period is T=1/(2.4×109 Hz)≈4.2×10−10 sT = 1/(2.4\times10^9\ \text{Hz}) \approx 4.2\times10^{-10}\ \text{s}. The wave travels the 3 m3\ \text{m} to the phone at c=3.0×108 m/sc = 3.0\times10^8\ \text{m/s}, arriving after t=3.0 m/(3.0×108 m/s)=1.0×10−8 st = 3.0\ \text{m} / (3.0\times10^8\ \text{m/s}) = 1.0\times10^{-8}\ \text{s}. The wavelength in air is λ=c/f=(3.0×108 m/s)/(2.4×109 Hz)=0.125 m=12.5 cm\lambda = c/f = (3.0\times10^8\ \text{m/s})/(2.4\times10^9\ \text{Hz}) = 0.125\ \text{m} = 12.5\ \text{cm}. The phone detects the oscillating electric and magnetic fields of the wave.

Connection

This is Maxwell's unified electromagnetic field in action. The oscillating current in the router antenna produces a changing electric field EE around the antenna, which produces a changing magnetic field BB; that changing BB in turn produces a changing EE, so the pair propagates as a self-sustaining wave without any medium. The energy density carried by the wave is u=12ϵ0E2+12μ0B2u = \frac{1}{2}\epsilon_0 E^2 + \frac{1}{2\mu_0} B^2, showing that EE and BB are two inseparable components of one field. The phone's antenna responds to the local EE and BB of this unified field.

Bicycle dynamo: rotating magnet and induction

Scenario

A bicycle moves at 18 km/h=5.0 m/s18\ \text{km/h} = 5.0\ \text{m/s}. The wheel radius is 0.35 m0.35\ \text{m}, so the wheel turns at about 5.0/(2π×0.35)≈2.35.0/(2\pi \times 0.35) \approx 2.3 revolutions per second. A sidewall dynamo steps this up so its permanent magnet rotates at 20 Hz20\ \text{Hz} next to a coil of N=8000N = 8000 turns with area A=1.5 cm2=1.5×10−4 m2A = 1.5\ \text{cm}^2 = 1.5\times10^{-4}\ \text{m}^2. The magnetic field through the coil has peak value B0=0.20 TB_0 = 0.20\ \text{T}. The peak induced emf is E0=NAB0ω\mathcal{E}_0 = N A B_0 \omega, with ω=2πf=2π(20 Hz)≈126 rad/s\omega = 2\pi f = 2\pi(20\ \text{Hz}) \approx 126\ \text{rad/s}, giving E0≈8000×1.5×10−4×0.20×126≈6.0 V\mathcal{E}_0 \approx 8000 \times 1.5\times10^{-4} \times 0.20 \times 126 \approx 6.0\ \text{V}. The dynamo delivers about 3 W3\ \text{W} to the headlamp.

Connection

The rotating magnet makes the magnetic flux through the coil change. According to the unified electromagnetic field, a changing magnetic field BB is accompanied by a circulating electric field EE; this induced EE drives the current that lights the lamp. The same coupled field explains why a dynamo and an electric motor are one device run in opposite directions: a current creates BB, and a changing BB creates EE. Here the unified model replaces separate magnetic and electric effects with a single field whose components transform into each other.

Induction hob: eddy currents in the pot bottom

Scenario

An induction hob has a coil under the glass. The coil carries an alternating current at 25 kHz25\ \text{kHz} and the hob delivers 2000 W2000\ \text{W} to a pot. The rapidly changing magnetic field BB (peak about 0.01 T0.01\ \text{T} at the pot bottom) induces eddy currents in the ferromagnetic base of the pot. To heat 1.0 L1.0\ \text{L} of water from 20 ∘C20\ ^\circ\text{C} to 100 ∘C100\ ^\circ\text{C} requires Q=mcΔT=(1.0 kg)(4186 J kg−1K−1)(80 K)=3.35×105 JQ = mc\Delta T = (1.0\ \text{kg})(4186\ \text{J kg}^{-1}\text{K}^{-1})(80\ \text{K}) = 3.35\times10^5\ \text{J}. At 2000 W2000\ \text{W} this takes t=Q/P=3.35×105/2000≈168 st = Q/P = 3.35\times10^5/2000 \approx 168\ \text{s}, about 2.8 min2.8\ \text{min}, matching a real hob. The glass stays cool because it is not electrically conducting.

Connection

The coil's alternating current produces a time-varying magnetic field BB. Because BB reverses 25 00025\,000 times per second, dB/dtdB/dt is large, and the unified electromagnetic field requires an accompanying electric field EE inside the pot. That EE drives eddy currents, which dissipate energy as heat. This is a direct use of the unified model: an electric field appears where there is no battery and no wire, purely because the magnetic field is changing. It also shows that EE and BB are not independent but two aspects of one field.