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Microwave Devices E511 Lecture 2 Amr Al.Awamry

Microwave Devices Lecture02

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Page 1: Microwave Devices Lecture02

Microwave Devices E511Lecture 2

Amr Al.Awamry

Page 2: Microwave Devices Lecture02

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 Lecture02

Plan waves in Lossless Medium

Helmholtz Equation in x direction

Leads to

Leads to

Phase velocity condition

Magnetic field

wavelength

Page 4: Microwave Devices Lecture02

Plan waves in general lossy Medium

Conductivity NOT equal ZERO

In a lossy Dielectric

Magnetic Field

Page 5: Microwave Devices Lecture02

In Good conductor

Skin Depth

Page 6: Microwave Devices Lecture02

Plan wave summary in diff. media

Page 7: Microwave Devices Lecture02

General Plan wave Equation Solution

Page 8: Microwave Devices Lecture02

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 Lecture02

Enegry & Power

Page 10: Microwave Devices Lecture02

Enegry & Power cont.

where

Poynting Vector

Losses in Medium

Stored Energy

Page 11: Microwave Devices Lecture02

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