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EELE 3332 Electromagnetic II Microstrip Transmission Lines Islamic University of Gaza Electrical Engineering Department Dr. Talal Skaik 2013 1

EELE 3332 Electromagnetic II Microstrip Transmission Linessite.iugaza.edu.ps/tskaik/files/Microstrip.pdf · Dr. Talal Skaik 2012 IUG 11 Stripline The geometry is shown, it consists

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EELE 3332 – Electromagnetic II

Microstrip Transmission Lines

Islamic University of Gaza

Electrical Engineering Department

Dr. Talal Skaik

2013 1

2

Transmission lines

3

Microstrip

Microstrip transmission line. (a) Geometry. (b) Electric and magnetic field lines.

Microstrip line is one of the most popular types of planar

transmission lines because of ease of fabrication and integration with

other passive and active microwave devices.

The geometry is shown, it consists of a conductor of width W

printed on a grounded dielectric substrate of thickness h and relative

permittivity εr.

4

Microstrip

5

Microstrip

Since some of the field lines are in the dielectric region and some are

in air, (the dielectric region does not fill the air region above the strip

(y>h)), an effective dielectric constant εe is considered in the analysis.

The effective dielectric constant satisfies the relation and

it is dependent on the substrate thickness h, and conductor width W.

εe can be interpreted as the dielectric constant of a homogeneous

medium that replaces the air and dielectric regions of the microstrip, as

shown.

Dr. Talal Skaik 2012 IUG 6

Microstrip

1 e r

1 1 1

2 2 1 12 /

r re

h W

7

0

1 1 1

2 2 1 12 /

Given the dimensions of the microstrip line, the characteristic impedance

can be calculated as

60 8ln / 1

4Z =

120

/ 1.393 0

r re

e

e

h W

h Wfor W h

W h

W h

/ 1

.667 ln / 1.444

The velocity is calculated as

The propagation constant is =

e

e

for W hW h

cu

u c

Microstrip

8

0 r

2

For a given characterestic impedance Z and dielectric constant ,

the / ratio can be found as:

8 / 2

2

12 0.611 ln(2 1) ln( 1) 0.39 / 2

2

A

A

r

r r

W h

efor W h

eW

hB B B for W h

where

0

0

1 1 0.11A= 0.23

60 2 1

377

2

r r

r r

r

Z

BZ

Microstrip

Attenuation can be caused by dielectric loss and conductor loss.

If αd is attenuation constant due to dielectric loss, and αc is the

attenuation due to conductor loss, the total attenuation constant is:

α= αd + αc

Considering the microstrip as a quasi-TEM line, the attenuation due to

dielectric loss can be determined as:

9

Microstrip - Losses

00

( 1) tan 2 Np/m ,

2 ( 1)

where tan is the loss tangent of the dielectric.

The attenuation due to conductor loss is given approximately by:

r ed

e r

k fk

c

0

0

Np/m

where / 2 is the surface resistivity of the conductor.

sc

s

R

Z W

R

10

r

Example: Calculate the width and length of a microstrip line for a 50

characterestic impadance and a 90 phase shift at 2.5 GHz. The substrate

thickness is h=0.127 cm, with =2.2

o

0.

Microstrip - Example

0

0

We first find / for 50 , and initially guess that / 2.

3777.985

2

12 0.61/ 1 ln(2 1) ln( 1) 0.39 3.081

2

/ 2; otherwise we would use the e

Solution:

r

r

r r

W h Z W h

BZ

W h B B B

So W h

o

8

xpression for / 2.

, 3.081 0.391

1 1 1The effective dielectric constant is 1.87

2 2 1 12 /

The length for a 90 phase shift is found as

(90 )( /180)(3 10 )90

(2 )

r re

oo

e

e

W h

So W h cm

h W

l

l l lc f

2.19 cml

Dr. Talal Skaik 2012 IUG 11

Stripline

The geometry is shown, it consists of a thin conducting strip of width

W centered between two wide conducting ground planes of separation

h, and the entire region between the ground planes is filled with a

dielectric.

In practice, stripline is usually constructed by etching the centre

conductor on a grounded substrate of thickness h/2, and then covering

with another grounded substrate of the same thickness.

Notice that all fields exist within the dielectric substrate.

Dr. Talal Skaik 2012 IUG 12

Stripline

0 0

0

1The velocity is :

The propagation constant is =

30The characterestic impedance is: Z

0.441

where is the effective width of the centre conductor given by

r r

r

er

e

cu

u c

h

W h

W

W

2

0

0 0.35

0.35 / 0.35

These formulas assume a zero strip thickness, and are quoted as being

accurate to about 1% of the exact results.

* Notice that Z decreases as the str

e

Wfor

W h

Wh hW h for

h

ip width increases.W

Dr. Talal Skaik 2012 IUG 13

Stripline

0

0

0

0

Given the characterestic impedance Z , and height and permittivity ,

the strip width can be found by:

120

0.85 0.6 120

30 0.441

Z

r

r

r

r

h

x for ZW

h x for Z

where x

Dr. Talal Skaik 2012 IUG 14

Stripline - Losses

d

3

0

The attenuation due to dielectric loss is given by:

tan = Np/m (general for TEM waves) ,

2

The attenuation due to conductor loss is approximately:

2.7 10

30 ( )

r

s r

c

kk

u c

R Z

h t

0

0

0

for 120

Np/m 0.16

for 120

2 1 2with 1+ ln

0.414 1 4 1 0.5 ln

0.5 0.7 2

is the thickness of the strip

r

sr

A Z

RB Z

Z h

W h t h tA

h t h t t

h t WB

W t W t

where t

.

15

Microstrip applications

16

Low Pass Filters

17

Bandpass Filters

18

Microstrip Antennas

Dr. Talal Skaik 2012 IUG 19

Design tools - txline software

Example: Calculate the width and length of a microstrip line for a 50 Ω

characteristic impedance and a 90o phase shift at 2.5 GHz. The substrate

thickness is h=0.127cm, with εr=2.20. Use txline software to design.