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Microwave Devices E511 Lecture 2 Amr Al.Awamry

Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

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Page 1: Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

Microwave Devices E511Lecture 2

Amr Al.Awamry

Page 2: Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

Agenda Plan waves in Lossless MediumPlan waves in general lossy

MediumIn Good conductorGeneral Plan wave Equation

SolutionPlan wave PolarizationEnegry & PowerReflection and transmission

coefficients

Page 3: Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

Plan waves in Lossless Medium

Helmholtz Equation in x direction

Leads to

Leads to

Phase velocity condition

Magnetic field

wavelength

Page 4: Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

Plan waves in general lossy Medium

Conductivity NOT equal ZERO

In a lossy Dielectric

Magnetic Field

Page 5: Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

In Good conductor

Skin Depth

Page 6: Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

Plan wave summary in diff. media

Page 7: Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

General Plan wave Equation Solution

Page 8: Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

Plan wave Polarization

If E1 and E2 are REALThen it’s called Linear Polarization

If E2 = jE1 then it’s called LHCP

If E2 = -jE1 then it’s called RHCP

Page 9: Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

Enegry & Power

Page 10: Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

Enegry & Power cont.

where

Poynting Vector

Losses in Medium

Stored Energy

Page 11: Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan

Reflection and transmission coefficients

( )

1( ) ( )

z zx i r

z zy i r

E z E e E e

H z E e E e

r

i

E

E