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# Review of Waves - PowerPoint PPT Presentation

Review of Waves. Properties of electromagnetic waves in vacuum : Waves propagate through vacuum (no medium is required like sound waves) All frequencies have the same propagation speed, c in vacuum.

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Review of Waves

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## Review of Waves

Properties of electromagnetic waves in vacuum:

Waves propagate through vacuum (no medium is required like sound waves)

All frequencies have the same propagation speed, c in vacuum.

Electric and magnetic fields are oriented transverse to the direction of propagation. (transverse waves)

Waves carry both energy and momentum.

E and B fields in waves and Right Hand Rule:

f+ solution

Wave propagates in E x B direction

f- solution

Special Case Sinusoidal Waves

Wavenumber and wavelength

These two contain the same information

Special Case Sinusoidal Waves

Introduce

Different ways of saying the same thing:

Polarizations

We picked this combination of fields: Ey - Bz

Could have picked this combination of fields: Ez - By

These are called plane polarized. Fields lie in plane

Which of the following are valid EM waves?

1.

Yes

No

A.Yes

B. No

2.

3.

A.Yes

B. No

4.

What direction is this wave propagating in?

Y

Z

X

None of above

z

Direction of propagation

Ex

.

Wave Vector

By , Bz

y

Energy Density and Intensity of EM Waves

Energy density associated with electric and magnetic fields

For a wave:

Thus:

Units: J/m3

Energy density in electric and magnetic fields are equal for a wave in vacuum.

We now want to expand the picture in the following way:

EM waves propagate in 3D not just 1D as we have considered.

- Diffraction - waves coming from a finite source spread out.

EM waves propagate through material and are modified.

- Dispersion - waves are slowed down by media, different

frequency waves travel with different speeds

- Reflection - waves encounter boundaries between media.

Some energy is reflected.

- Refraction - wave trajectories are bent when crossing from

one medium to another.

EM waves can take multiple paths and arrive at the same point.

- Interference - contributions from different paths add or

cancel.

Waves emanating from a point source

Wave crests

When can one consider waves to be like particles following a trajectory?

Motion of crests

Direction of power flow

• Wave model: study solution of Maxwell equations.

Most complete classical description. Called physical optics.

• Ray model: approximate propagation of light as that of particles following specific paths or “rays”. Called geometric optics.

• Quantum optics: Light actually comes in chunks called photons

What is the difference?

Diffraction.

Comparable to opening size

Much smaller than opening size

Diffraction

Propagation of light through dielectric media

In a dielectric the Electric field causes molecules/atoms to become polarized.

Molecules align with field

Medium becomes “polarized”

What happens when the electric field oscillates in time?

A current is induced.

How is the Ampere-Maxwell Law modified?

Dielectric

For S2 there is both displacement current and real current

Real current given by dielectric constant

Electric flux

Dielectric constant

In a dielectric material

Bottom Line:

Dielectric constant

Replace

by

Static dielectric constants

To complicate matters, dielectric constant depends on frequency.

Dielectric function depends on frequency

Consequences for EM Plane waves

Propagation speed changes in a material

Refraction

Ratio of E to B changes

Reflection

For sinusoidal waves the following is still true

Index of refraction

For sinusoidal waves the following is still true

Frequency is the same in both media

Wavelength changes

A light wave travels through three transparent materials of equal thickness. Rank in order, from the largest to smallest, the indices of refraction n1, n2, and n3.

• n1 > n2 > n3

• n2 > n1 > n3

• n3 > n1 > n2

• n3 > n2 > n1

• n1 = n2 = n3

Example: Optical fiber

d

Fused silica: n=1.48

Vacuum wavelength l = 1550 nm

Wavelength in fiber l/n = 1045nm

D = 10 mm

P=1mW inside fiber

I=P/A=?

E=?

In vacuum

Rays bounce back and forth

Reflection from surface

incident

transmitted

reflected

Region 1

Region 2

Reflection coefficient

What if

“Index matched”

Ey, Bz

How to calculate reflection

At x=0 fields are continuous

x

region 1

0

region 2

For x<0

incident

For x>0

reflected

transmitted

Continuity of Ey at x=0

x<0

x>0

Continuity of Bz at x=0

x<0

x>0

Solve for reflected & transmitted pulses

Example: what fraction of power is reflected at boundary between glass and air?

Reflection coefficient

Air: n1=1.0003Glass: n2 =1.5

ratio of reflected to incident electric field amplitude

I=Power/Area

ratio of reflected to incident intensity

Suppose the wave was incident on the boundary from the glass side

incident

transmitted

reflected

Region 1

Region 2

n1=1.5

n2=1.0

What is reflection coefficient?

incident

transmitted

reflected

Region 1

Region 2

n1=1.5

n2=1.0

What is reflection coefficient?

r=0

r =.2

C. r =-.2

D. r =5

Region 2 has higher velocity

Region 2 has lower velocity

What if

Same as for reflection from a conductor

Interference in 1 Dimension

incident

Incident and reflected fields add (superposition)

reflected

incident

reflected

Incident and reflected waves will interfere, changing the peak electric field at different points

Case #1: no reflection r=0.

No interference,

E plotted versus x for several values of t

E plotted versus t for a single value of x.

Same peak value independent of x

Traveling wave

Case #2: total reflection r= -1.

Anti-nodes

E plotted versus x for several values of t

nodes

How far apart are the nodes?

Anti-nodes?

What is peak E?

Case #3: total reflection r= +1.

E plotted versus x for several values of t

= VSWR

Emax

Emin

Case #4: partial reflection r= -0.5

E plotted versus x for several values of t

How far apart are the minima?

The Maxima?

What is peak E?

When reflection is not total there are still local maxima and minima.

Voltage Standing Wave Ratio

Pronounced “vizwarr”

Half Wavelength Window

Eliminates Reflection

incident

incident

transmitted

reflected

Region 1

Region 2

Region 1’

D

When dielectric #2 is an integer number

of half-wavelengths thick, no reflection

CVD diamond window

Manufactured by elementsix

http://www.e6.com/wps/wcm/connect/E6_Content_EN/Home

Summary

Waves are modified by dielectric constant of medium, k.

All our Maxwell equations are valid provided we replace

3. Speed of waves is lowered. (Index of refraction - n)

4. Frequency of wave does not change in going from one medium to another. Wavelength does.

5. Waves are reflected at the boundary between two media.

(Reflection coefficient)

= VSWR

6. Reflected waves interfere with incident waves.

Distance between interference maxima/minima

Ratio of maximum peak field to minimum peak field

(Voltage standing wave ratio)

Solution of the Wave equation

Where f+,- are any two functions you like,

and

is a property of space.

Represent forward and backward propagating wave (pulses). They depend on how the waves were launched

Shape of pulse determined by source of wave.

Speed of pulse determined by medium

What is the magnetic field of the wave?

Notice minus sign

Ey (V/m)

The graph at the top is the history graph at x = 4 m of a wave traveling to the right at a speed of 2 m/s. Which is the history graph of this wave at x = 0 m?

What is the frequency of this traveling wave?

• 0.1 Hz

• 0.2 Hz

• 2 Hz

• 5 Hz

• 10 Hz

What is the phase difference between the crest of a wave and the adjacent trough?

• 0

• π

• π/4

• π/2

• 3 π/2