electromagnetism inel 4152 ch 10 sandra cruz-pol, ph. d. ece uprm mayag ü ez, pr

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Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayagüez, PR

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Page 1: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

ElectromagnetismINEL 4152

Ch 10

Sandra Cruz-Pol, Ph. D.ECE UPRM

Mayagüez, PR

Page 2: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Outline Plane Wave types

general, lossy, lossless…. Power in a Wave Applications and Concepts

Page 3: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Page 4: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Plane waves10.1

Page 5: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

A wave!

Start taking the curl of Faraday’s law

Then apply the vectorial identity

And you’re left withAAA 2)(

ss HjE

Page 6: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

A Wave

022 EE

Let’s look at a special case for simplicity without loosing generality:• The electric field has only an x-component• The field travels in z direction

Then we have

zo

zo eEe EE(z)

tzE

'

issolution general whose

),(

Page 7: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

To change back to time domain

From phasor

…to time domain

)()( jzo

zoxs eEeEzE

xzteEtzE zo

)cos(),(

Page 8: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Plane wave Propagation in Several Media

10.3-10.6

Page 9: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Several Cases of Media

1. Free space

2. Lossless dielectric

3. Lossy dielectric (general)

4. Good Conductor

Recall: Permittivity eo=8.854 x 10-

12 [F/m]

Permeability mo= 4p x 10-7

[H/m]

Page 10: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

1. Free space

There are no losses, e.g.

Let’s define The phase of the wave The angular frequency Phase constant The phase velocity of the wave The period and wavelength In what direction does it moves?

Page 11: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Where does it moves?

Pick 3 times: Plot

Cruz-Pol, Electromagnetics UPRM

Page 12: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

3. General Case (Lossy Dielectrics)

In general, we had and

From these we obtain

So , for a known material and frequency, we can find = +g a jb

112

2

xzteEtzE zo

)cos(),(

j

2

2Re

22222

222

11

2

2

Page 13: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

SummaryAny medium Lossless

medium (s=0)

Low-loss medium(e”/e’<1/100)

Good conductor(e”/e’>100)

Units

a [Np/m]

b [rad/m]

h

up

l

/w b [m/s]

[m]

**In free space; eo =8.85 x 10-12 F/m mo=4p x 10-7 H/m

11

2

2

j

j

f

u p

1

2

f

u p

1

)1( j

11

2

2

rr

c

Page 14: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Example: Water

Cruz-Pol, Electromagnetics UPRM

Page 15: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Permittivity of water vs. freq.

http://www.random-science-tools.com/electronics/water_dielectric.htm

Page 16: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Example Water @ 60Hz, (Low freq.)

Find a , b and h For distilled water

For sea water

Attenuation const.

Phase constant

Page 17: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Example Water @ 10GHz, (microwaves)

Find a , b and h For distilled water

For sea water

2

Attenuation const.

Phase constant

Page 18: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Intrinsic Impedance, h If we divide E by H, we get units of ohms and

the definition of the intrinsic impedance of a medium at a given frequency.

][ ||

||

j

j

H

E

*Not in-phase for a lossy medium

Page 19: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Applet

Cruz-Pol, Electromagnetics UPRM

See Applet by Daniel Roth at

http://fipsgold.physik.uni-kl.de/software/java/oszillator/index.html

Page 20: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Note…

E and H are perpendicular to one another Travel is perpendicular to the direction of

propagation The amplitude is related by the impedance And so is the phase

Page 21: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Loss Tangent

If we divide the conduction current by the displacement current

tangentosstan lEj

E

J

J

s

s

ds

cs

Page 22: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Relation between tanq and ec

EjjEjEH

1

Ej c

'''1

isty permittivicomplex The

jjc

'

"tanas also defined becan tangent loss The

Page 23: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

2. Lossless dielectric

Substituting in the general equations:

)or ,,0( oror

o

u

0

21

,0

Page 24: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Review: 1. Free Space

Substituting in the general equations:

mAyztE

tzH

mVxztEtzE

o

o

o

/ˆ)cos(),(

/)cos(),(

) ,,0( oo

3771200

21

/,0

o

o

o

oo

cu

c

Page 25: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

4. Good Conductors

Substituting in the general equations:

]/[ˆ)45cos(),(

]/[)cos(),(

mAyzteE

tzH

mVxzteEtzE

oz

o

o

zo

) ,,( oro

o

u

45

22

2

Is water a good conductor???

Page 26: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

SummaryAny medium Lossless

medium (s=0)

Low-loss medium(e”/e’<1/100)

Good conductor(e”/e’>100)

Units

a [Np/m]

b [rad/m]

h

uc

l

/w b [m/s]

[m]

**In free space; eo =8.85 x 10-12 F/m mo=4p x 10-7 H/m

11

2

2

j

j

f

u p

1

2

f

u p

1

)1( j

11

2

2

rr

c

Page 27: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Ejemplo

In a free space,

Find Jd and E

Cruz-Pol, Electromagnetics UPRM

Page 28: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Skin depth, d

Is defined as the depth at which the electric amplitude is decreased to 37%

/1at

%)37(37.01

1

zee

ez

[m] /1

We know that a wave attenuates in a lossy medium until it vanishes, but how deep does it go?

]/[)cos(),( mVxzteEtzE zo

Page 29: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Microwave OvenMost food are lossy media at

microwave frequencies, therefore EM power is lost in the food as heat.

Find depth of penetration for potato which at 2.45 GHz has the complex permittivity given.

The power reaches the inside as soon as the oven in turned on!

)130( joc

Page 30: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Short Cut!

You can use Maxwell’s or use

where k is the direction of propagation of the wave, i.e., the direction in which the EM wave is traveling (a unitary vector).

HkE

EkH

ˆ

ˆ1

Page 31: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Waves - Summary

Static charges > static electric field, E Steady current > static magnetic field, H Static magnet > static magnetic field, H

Time-varying current > time varying E(t) & H(t) that are interdependent > electromagnetic wave

Time-varying magnet > time varying E(t) & H(t) that are interdependent > electromagnetic wave

Page 32: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

EM waves don’t need a medium to propagate

Sound waves need a medium like air or water to propagate

EM waves don’t. They can travel in free space in the complete absence of matter.

Look at a “wind wave”; the energy moves, the plants stay at the same place.

Page 33: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Exercises: Wave Propagation in Lossless materials

A wave in a nonmagnetic material is given by

Find:

(a) direction of wave propagation,

(b) wavelength in the material

(c) phase velocity

(d) Relative permittivity of material

(e) Electric field phasor

[mA/m])510cos(50ˆ 9 ytzH

[V/m]57.12ˆ 5 yjexE

Answer: +y, l=1.26m, up= 2x108 m/s, 2.25,

Page 34: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Power and Poynting Vector

10.7-10.8

Page 35: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Power in a wave

A wave carries power and transmits it wherever it goes

The power density per area carried by a wave is given by the Poynting vector.

Page 36: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Poynting Vector Derivation

Start with E dot Ampere’s

Apply vector identity

And end up with:

EHHEEH

BAABBA

:case in thisor

t

EEEEHE

t

EEHE

t

EEEHEH

2

2

2

1

Page 37: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Poynting Vector Derivation…

Substitute Faraday in 1rst term

t

EEEH

t

HH

2

2

2

1

t

HH

t

HH

2

:function square of derivativein As

t

EEHE

t

H

2

22

22

HEEH

(-) sit' order, invert the if and

222

22E

t

H

t

EHE

Rearrange

Page 38: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Poynting Vector Derivation…

Taking the integral wrt volume

Applying Theorem of Divergence

Which means that the total power coming out of a volume is either due to the electric or magnetic field energy variations or is lost in ohmic losses.

Total power across surface of volume

Rate of change of stored energy in E or H

Ohmic losses due to conduction current

Page 39: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Power: Poynting Vector

Waves carry energy and information Poynting says that the net power flowing out of a

given volume is = to the decrease in time in energy stored minus the conduction losses.

][W/m 2HE

P

Represents the instantaneous power density vector associated to the electromagnetic wave.

Page 41: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cellphone power radiation

Cruz-Pol, Electromagnetics UPRM

Source: AnSys= Fred German

Page 42: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Time Average Power density

The Poynting vector averaged in time is

For the general case wave:

*

00

Re2

111ss

TT

ave HEtdHET

tdT

PP

Page 43: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Total Power in W

The total power through a surface S is

Note that the units now are in Watts Note that power nomenclature, P is not cursive. Note that the dot product indicates that the surface

area needs to be perpendicular to the Poynting vector so that all the power will go thru. (give example of receiver antenna)

Page 44: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

PE 10.7

In free space, solar TEM wave at some latitude & season can be measured to be H=0.2 cos (wt-bx) z A/m. Find the total power passing through a solar panel of side 10cm on plane

square plate at

Answer; Ptot = =53mW

Hz

Ey

x

Answer; Ptot = 0mW!

Page 45: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Solar Panels

http://www.altenergymag.com/emagazine.php?

issue_number=05.08.01&article=gonzalez

Optimum inclination of solar panels for maximum power transmission depends on geographical location.

Page 46: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Exercises: Power2. A 5GHz wave traveling In a nonmagnetic medium with

er=9 is characterized by Determine the direction of wave travel and the average power density carried by the wave

Answer:

[V/m])cos(2ˆ)cos(3ˆ xtzxtyE

Page 47: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

TEM wave

Transverse ElectroMagnetic = plane wave

There are no fields parallel to the direction of propagation,

Only perpendicular (=transverse). If have an electric field Ex(z)

…then must have a corresponding magnetic field Hy(z) The direction of propagation is

Page 48: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Polarization:Why do we care?? Antenna applications –

Antenna can only TX or RX a polarization it is designed to support.• Straight wires, square waveguides, and similar rectangular systems support

linear waves (polarized in one direction) • Round waveguides, helical or flat spiral antennas produce circular or elliptical

waves. Remote Sensing and Radar Applications –

Many targets will reflect or absorb EM waves differently for different polarizations.

Using multiple polarizations can give more information and improve results.

Absorption applications – Human body, for instance, will absorb waves with E oriented from

head to toe better than side-to-side, esp. in grounded cases. Also, the frequency at which maximum absorption occurs is different for these two polarizations. This has ramifications in safety guidelines and studies.

Page 49: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Page 50: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Outline Origin Maxwell Equations explain waves Phasors and Time Harmonic fields

Maxwell eqs for time-harmonic fields Cases

general, lossy, lossless…. Wave Power Applications and Concepts

Page 51: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Cell phone & brain Computer model for Cell phone

Radiation inside the Human Brain SAR=Specific Absorption Rate [W/Kg]

FCC limit 1.6W/kg, ~.2mW/cm2 for 30mins

http://www.ewg.org/cellphoneradiation/Get-a-Safer-Phone/Samsung/Impression+%28SGH-a877%29/

Page 52: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Human absorption

30-300 MHz is where the human body absorbs RF energy most efficiently

http://handheld-safety.com/SAR.aspx http://www.fcc.gov/Bureaus/Engineering_Technology/Docume

nts/bulletins/oet56/oet56e4.pdf

http://www.rfcafe.com/references/electrical/fcc-maximum-permissible-exposure.htm

* The FCC limit in the US for public exposure from cellular telephones at the ear level is a SAR level of 1.6 watts per kilogram (1.6 W/kg) as averaged over one gram of tissue.

Cruz-Pol, Electromagnetics UPRM

Page 53: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

ICNIRP= Intl Commission of Non-ionizing radiation protection

Page 54: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Exercise: Cellphone Tower Safe Power Level

At microwave frequencies, the power density considered safe for humans is 1 mW/cm2.(SAR varies by frequency and country) A cellphone tower radiates a wave with an electric field amplitude E that decays with distance as |E(R)|=3000/R [V/m], where R is the distance in meters. What is the radius of the unsafe region?

Answer: 34.54 m

Page 55: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Radiación en Teléfonos móviles

6 Tips para Protegerte: 1. Mantén las llamadas cortas.

2. Mantén distancia de 1“ (2.5 cm) del cuerpo)

3. Usa el cable auricular

4. Usa bocina altoparlante,

5. Apaga el bluetooth, GPS y WiFi cuando no lo estés usando

6. Envía texto en vez

7. *Coteja el nivel de radiación en tu modelo. Depende de la región. Los mismos modelos en Europa emiten menos radiación debido a exigencias de sus leyes. Busca en sarvalues.com SAR levels

En 2011, la Organización Mundial de la Salud de la ONU clasificó a los teléfonos celulares en Categoría de Peligro de Cáncer, a pesar de que producen radiación no-ionizante

Page 56: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Radar bandsBand Name

Nominal FreqRange Specific Bands Application

HF, VHF, UHF3-30 MHz0, 30-300 MHz, 300-

1000MHz

138-144 MHz216-225, 420-450 MHz890-942

TV, Radio,

L 1-2 GHz (15-30 cm) 1.215-1.4 GHz Clear air, soil moist

S 2-4 GHz (8-15 cm) 2.3-2.5 GHz2.7-3.7>

Weather observationsCellular phones

C 4-8 GHz (4-8 cm) 5.25-5.925 GHzTV stations, short range

Weather

X 8-12 GHz (2.5–4 cm) 8.5-10.68 GHz

Cloud, light rain, airplane weather. Police radar.

Ku 12-18 GHz 13.4-14.0 GHz, 15.7-17.7 Weather studies

K 18-27 GHz 24.05-24.25 GHz Water vapor content

Ka 27-40 GHz 33.4-36.0 GHz Cloud, rain

V 40-75 GHz 59-64 GHz Intra-building comm.

W 75-110 GHz 76-81 GH, 92-100 GHz Rain, tornadoes

millimeter 110-300 GHz Tornado chasers

Page 57: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Electromagnetic Spectrum

Page 58: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Radares UPRM

Cruz-Pol, Electromagnetics UPRM

Page 59: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Decibel Scale

In many applications need comparison of two powers, a power ratio, e.g. reflected power, attenuated power, gain,…

The decibel (dB) scale is logarithmic

Note that for voltages, fields, and electric currents, the log is multiplied by 20 instead of 10.

2

12

2

21

2

1

2

1

log20log10log10][V

V

/RV

/RV

P

PdBG

P

P G

Page 60: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Attenuation rate, A

Represents the rate of decrease of the magnitude of Pave(z) as a function of propagation distance`

Page 61: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Submarine antenna

A submarine at a depth of 200m uses an antenna array to receive signal transmissions at 1kHz.

Determine the power density incident upon the submarine antenna due to the EM wave with |Eo|= 10V/m.

[At 1kHz, sea water has er=81, =4].

At what depth the amplitude of E has decreased to 1% its initial value at z=0 (sea surface)?

Page 62: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

SummaryAny medium Lossless

medium (s=0)

Low-loss medium(e”/e’<1/100)

Good conductor(e”/e’>100)

Units

a [Np/m]

b [rad/m]

h

uc

l

/w b [m/s]

[m]

**In free space; eo =8.85 x 10-12 F/m mo=4p x 10-7 H/m

11

2

2

j

j

f

u p

1

2

f

u p

1

)1( j

11

2

2

rr

c

Page 63: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Exercise: Lossy media propagation

For each of the following determine if the material is low-loss dielectric, good conductor, etc.

(a) Glass with mr=1, er=5 and s=10-12 S/m at 10 GHZ

(b) Animal tissue with mr=1, er=12 and s=0.3 S/m at 100 MHZ

(c) Wood with mr=1, er=3 and s=10-4 S/m at 1 kHZ

Answer:(d) low-loss, = 8.4a x10-11 Np/m, =b 468 r/m, = 1.34 l cm, up=1.34x108, hc=168

W(e) general, =a 9.75, =12, =52 b l cm, up=0.5x108 m/s, hc=39.5+j31.7 W

(f) Good conductor, = 6.3a x10-4, = 6.3b x10-4, = 10l km, up=0.1x108, hc=6.28(1+j) W

Page 64: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Cruz-Pol, Electromagnetics UPRM

Who was NikolaTesla?

Find out what inventions he made His relation to Thomas Edison Why is he not well known?

http://www.youtube.com/watch?v=i-j-1j2gD28&feature=related

Page 65: Electromagnetism INEL 4152 Ch 10 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR

Pure Water is blue

Is turquoise blue due to its electromagnetic spectrum emission

http://ece.uprm.edu/~pol/OceanBlue

Cruz-Pol, Electromagnetics UPRM