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Maxwell Equations: Electromagnetic Waves

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11/6/17 1 Maxwell Equations: Electromagnetic Waves Maxwell’s Equations contain the wave equation The velocity of electromagnetic waves: c = 2.99792458 x 10 8 m/s The relationship between E and B in an EM wave Energy in EM waves: the Poynting vector x z y
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Page 1: Maxwell Equations: Electromagnetic Waves

11/6/171

Maxwell Equations: Electromagnetic Waves

Maxwell’s Equations contain the wave equation

The velocity of electromagnetic waves:

c = 2.99792458 x 108 m/s

The relationship between E and B in an EM wave

Energy in EM waves: the Poynting vector

x

z

y

Page 2: Maxwell Equations: Electromagnetic Waves

11/6/172

The equations so far.....

Gauss’ Law for E Fields Gauss’ Law for B Fields

Faraday’s Law Ampere’s Law

Page 3: Maxwell Equations: Electromagnetic Waves

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A problem with Ampere’s Law•Time dependent situation: current flows in the wire as the capacitor charges up or down.

Consider a wire and a capacitor. C is a loop.

Page 4: Maxwell Equations: Electromagnetic Waves

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Maxwell’s Displacement Current, Id

Page 5: Maxwell Equations: Electromagnetic Waves

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Calculating Displacement CurrentConsider a parallel platecapacitor with circular plates of radius R. If charge is flowing onto one plate and off the other plate at a rate I = dQ/dt what is Id ?

•The displacement current is not a current. It represents magnetic fields generated by time varying electric fields.

Page 6: Maxwell Equations: Electromagnetic Waves

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Calculating the B fieldExample

Page 7: Maxwell Equations: Electromagnetic Waves

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Maxwell’s Equations (1865)

in Systeme International (SI or mks) units

Page 8: Maxwell Equations: Electromagnetic Waves

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Maxwell’s Equations (Free Space)Note the symmetry of Maxwell’s Equations in free space, when no charges or currents are present

h is the variable that is changing in space (x) and time (t). v is the velocity of the wave.

We can predict the existence of electromagnetic waves. Why? Because the wave equation is contained in these equations. Remember the wave equation.

Page 9: Maxwell Equations: Electromagnetic Waves

11/6/17 9

Review of Waves from MechanicsThe one-dimensional wave equation:

has a general solution of the form:

A solution for waves traveling in the +x direction is:

Page 10: Maxwell Equations: Electromagnetic Waves

11/6/1710

Four Step Plane Wave Derivation

Example:

Step 2 Apply Faraday’s Law to infinitesimal loop in x-zplane

Step 1 Assume we have a plane wave propagating in z(i.e. E, B not functions of x or y)

x

z

y

z1 z2

Ex Ex

∆Z

∆x

By

Page 11: Maxwell Equations: Electromagnetic Waves

11/6/1711

Four Step Plane Wave Derivation

Step 3 Apply Ampere’s Law to an infinitesimal loop in the y-z plane: x

z

y

z1 z2

By

∆Z

∆yBy

Ex

Step 4: Use results from steps 2 and 3 to eliminate By

Page 12: Maxwell Equations: Electromagnetic Waves

11/6/1712

Velocity of Electromagnetic WavesWe derived the wave equation for Ex:

The velocity of electromagnetic waves in free space is:

Putting in the measured values for µ0 & ε0, we get:

This value is identical to the measured speed of light! We identify light as an electromagnetic wave.

Page 13: Maxwell Equations: Electromagnetic Waves

11/6/1713

Electromagnetic Spectrum

~1850: infrared, visible, and ultraviolet lightwere the only forms of electromagnetic waves known.

Visible light (human eye)

Page 14: Maxwell Equations: Electromagnetic Waves

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Electro-magneticSpectrum

Page 15: Maxwell Equations: Electromagnetic Waves

Sunscreen Absorbs UV

11/6/1715

http://upload.wikimedia.org/wikipedia/commons/thumb/0/0d/UV_and_Vis_Sunscreen.jpg/800px-UV_and_Vis_Sunscreen.jpg

Page 16: Maxwell Equations: Electromagnetic Waves

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What a Bee Sees:

Page 17: Maxwell Equations: Electromagnetic Waves

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Wien’s Displacement Law

Page 18: Maxwell Equations: Electromagnetic Waves

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How is B related to E?

where

We derived the wave equation for Ex:

We could have derived for By:

How are Ex and By related in phase and magnitude?Consider the harmonic solution:

Page 19: Maxwell Equations: Electromagnetic Waves

11/6/1719

E & B in Electromagnetic WavesPlane Wave:

where:

x

z

y

where are the unit vectors in the (E,B) directions.

The direction of propagation is given by the cross product

Nothing special about (Ex,By); eg could have (Ey, -Bx)Note cyclical relation:

Page 20: Maxwell Equations: Electromagnetic Waves

11/6/1720

Energy in Electromagnetic WavesElectromagnetic waves contain energy. We know the

energy density stored in E and B fields:

The Intensity of a wave is defined as the average power (Pav=uav/Δt) transmitted per unit area = average energy density times wave velocity:

• For ease in calculation define Z0 as:

u Ec

E uB E= = =12

12

2

20

02

µεIn an EM wave, B = E/c

The total energy density in an EM wave = u, where

Page 21: Maxwell Equations: Electromagnetic Waves

11/6/1721

The Poynting VectorThe direction of the propagation of the

electromagnetic wave is given by:This energy transport is defined by the Poynting

vector S as:

The intensity for harmonic waves is then given by:

S has the direction of propagation of the waveThe magnitude of S is directly related to the energy being transported by the wave

Page 22: Maxwell Equations: Electromagnetic Waves

11/6/1722

Characteristics

Sxz

Page 23: Maxwell Equations: Electromagnetic Waves

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Summary of Electromagnetic Radiation

combined Faraday’s Law and Ampere’s Law– time varying B-field induces E-field– time varying E-field induces B-field

• E-field and B-field are perpendicular• energy density

•• Poynting Vector describes power flow

• units: watts/m2

E

BS


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