Electric and Magnetic Fields

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ECE390L17201024.pdf

10/26/2020

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COLLEGE OF ENGINEERING School of Electrical Engineering and Computer Science

ECE 390 – Electric & Magnetic Fields L17 – Wave Reflection and Transmission (8.1-8.2)

Fall 2020 T. Weller

School of EECS – ECE 390

Today’s Topics

• Wave reflection and transmission at normal incidence

• Snell’s law

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Signal Refraction at Boundaries

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Radiation by antenna (Chapter 9)

Wave propagation in lossless medium (Chapter 7)

Wave propagation in lossy  medium (Chapter 7)

Antenna reception (Chapter 9)

Wave refraction across a  boundary (this chapter)

School of EECS – ECE 390

Normal and Oblique Incidence

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Normal Incidence

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We can use all the transmission‐line  concepts and techniques of Chapter  2 to analyze plane wave reflection  and transmission at interfaces  between dissimilar media 

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Modeling Normal Incidence

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Individual Waves

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Note ‒ sign

Note + sign

Note ‒ sign

School of EECS – ECE 390

Boundary Conditions

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Total fields

At the boundary z = 0:

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Boundary Conditions

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Solution gives:

School of EECS – ECE 390

Reflection and Transmission Coefficients

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Similar form  as for  transmission lines

Lossless and non‐magnetic material

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With Lossy Material • If Medium 2 is lossy (i.e.  > 0) then it will have a

complex wave impedance  • Consequently, the reflection coefficient  will be a

complex number • If  is

– Negative, then the reflected wave is 180 degrees out of phase with the incident wave

– Positive, then the reflected wave is in phase with the incident wave

– Complex, then the reflected wave is out of phase with the incident wave somewhere between 0 and +/- 180 degrees

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Power Transfer

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Medium 1

Medium 2

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Example 8‐3 (cont.)

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Example 8-3 (cont.)

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Snell’s Laws

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Angles of Incidence, Reflection & Refraction

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Nonmagnetic Media

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Index of refraction n:

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Refraction

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When the refraction angle is  90 degrees, the corresponding  incidence angle is called the  critical angle.

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