EE 30358

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EE 30358 Electromagnetic Fields and Waves II
TA Timothy VASEN tvasen_at_nd.edu
Instructor Arpad I. CSURGAY 268 Fitzpatrick
Hall acsurgay_at_nd.edu
Textbook Magdy F. Iskander Electromagnetic
Fields and Waves Chapters 5 to 9
Electromagnetic Waves
Lectures Tuesday/Thursday 1100
-1215 DeBartolo 129
Office hours
www.nd.edu/acsurgay/EMagII_2008
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Textbook 2.12 2.15
Wave Equation in Source Free Region
Time Harmonic Fields and Their Phasor
Representation
Uniform Plane Wave Propagation in Free Space
Polarization of Plane Waves
Textbook 3.8 3.12
Uniform Plane Wave Propagation in Conductive
Medium
Electromagnetic Power and Poynting Theorem
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Uniform Plane Wave Propagation in Free Space
MAXWELLS EQUATIONS FOR PHASORS
Propagation in z direction
GENERAL SOLUTION FOR PHASORS IN SPACE
Descartes coordinates
GENERAL SOLUTION IN SPACE-TIME
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PHASOR VECTORS IN SPACE
GENERAL SOLUTION IN SPACE-TIME
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Textbook 2.12 2.15
Wave Equation in Source Free Region
Time Harmonic Fields and Their Phasor
Representation
Uniform Plane Wave Propagation in Free Space
Polarization of Plane Waves
Textbook 3.8 3.12
Uniform Plane Wave Propagation in Conductive
Medium
Electromagnetic Power and Poynting Theorem
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Polarization of Plane Waves
LINEAR POLARIZATION
CIRCULAR POLARIZATION
ELLIPTICAL POLARIZATION
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Textbook 2.12 2.15
Wave Equation in Source Free Region
Time Harmonic Fields and Their Phasor
Representation
Uniform Plane Wave Propagation in Free Space
Polarization of Plane Waves
Textbook 3.8 3.12
Uniform Plane Wave Propagation in Conductive
Medium
Electromagnetic Power and Poynting Theorem
8
Uniform Plane Wave Propagation in Conductive
Medium
MEDIUM OF PROPAGATION IS HOMOGENEOUS, LINEAR AND
ISOTROPIC
CONDUCTIVE MEDIUM
FREE SPACE
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Uniform Plane Wave Propagation in Conductive
Medium
MAXWELLS EQUATIONS FOR PHASORS
Propagation in z direction
GENERAL SOLUTION FOR PHASORS IN SPACE
Descartes coordinates
GENERAL SOLUTION IN SPACE-TIME
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PHASOR VECTORS IN SPACE
GENERAL SOLUTION IN SPACE-TIME
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Textbook CHAPTER 5
NORMAL-INCIDENCE PLANE-WAVE REFLECTION AND
TRANSMISSION AT PLANE BOUNDARIES BETWEEN TWO
CONDUCTIVE MEDIA
5.1 INTRODUCTION
5.2 NORMAL-INCIDENCE PLANE-WAVE REFLECTION AND
TRANSMISSION AT PLANE BOUNDARIES BETWEEN TWO
CONDUCTIVE MEDIA
5.3 NORMAL-INCIDENCE PLANE-WAVE REFLECTION AT
PERFECTLY CONDUCTING PLANE
5.4 REFLECTION AND TRANSMISSION AT MULTIPLE
INTERFACES
5.5 REFLECTION COEFFICIENT AND TOTAL FIELD
IMPEDANCE
5.6 GRAPHICAL SOLUTION PROCEDURE USING THE SMITH
CHART
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5.1 INTRODUCTION
5.2 NORMAL-INCIDENCE PLANE-WAVE REFLECTION AND
TRANSMISSION AT PLANE BOUNDARIES BETWEEN TWO
CONDUCTIVE MEDIA
Transmitted wave
The wave is normally incident on a plane
interface separating two conductive media
Boundary conditions at
Reflected wave
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Plane wave propagation in a conductive medium
of electrical properties
The wave is normally incident on an infinite
interface separating two conductive media
Boundary condition at
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Textbook CHAPTER 5
NORMAL-INCIDENCE PLANE-WAVE REFLECTION AND
TRANSMISSION AT PLANE BOUNDARIES BETWEEN TWO
CONDUCTIVE MEDIA
5.1 INTRODUCTION
5.2 NORMAL-INCIDENCE PLANE-WAVE REFLECTION AND
TRANSMISSION AT PLANE BOUNDARIES BETWEEN TWO
CONDUCTIVE MEDIA
5.3 NORMAL-INCIDENCE PLANE-WAVE REFLECTION AT
PERFECTLY CONDUCTING PLANE
5.4 REFLECTION AND TRANSMISSION AT MULTIPLE
INTERFACES
5.5 REFLECTION COEFFICIENT AND TOTAL FIELD
IMPEDANCE
5.6 GRAPHICAL SOLUTION PROCEDURE USING THE SMITH
CHART
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Plane wave propagation in a conductive medium
of electrical properties
The wave is normally incident on an infinite
interface separating two conductive media
Boundary condition at
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Perfectly conductive medium
Wave impedance
Appendix C p. 725 - 726
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PHASOR VECTORS IN SPACE
SOLUTION IN SPACE-TIME
Z 0
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Home work problems
Textbook Chapter 5 page 427 - 428
Problems 1, 2, 3, 4, 5,
TA Timothy VASEN tvasen_at_nd.edu
Office hours
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