eele 3332 electromagnetic ii chapter 11...

19
EELE 3332 Electromagnetic II Chapter 11 Transmission Lines Islamic University of Gaza Electrical Engineering Department Dr. Talal Skaik 2012 1

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EELE 3332 – Electromagnetic II

Chapter 11

Transmission Lines

Islamic University of Gaza

Electrical Engineering Department

Dr. Talal Skaik

2012 1

2

11.5 The Smith Chart

The Smith Chart is a graphical tool for analyzing transmission

lines.

The Smith Chart is made up of circles and arcs of circles.

The circles are called “constant resistance circles”

The arcs are “constant reactance circles”

The combination of intersecting circles and arcs inside the chart

allow us to locate the normalized impedance and then to find the

impedance anywhere on the line.

We will assume lossless transmission lines. (Zo=R0)

The Smith Chart is constructed within a circle of unit radius (|Γ|≤1).

Where Γr and Γi are the real and imaginary parts of Γ. 3

The Smith Chart

| | r ij

4

The Smith Chart

L

L

0

For the load impedance Z , the normalized impedance is:

Z

Z

L

L

z

z r jx

Smith Chart is normalized so that all impedances are normalized to the

characteristic impedance Z0. (Hence, it can be used for any line)

r-circles x-circles Resistance Circles

Reactance Circles

5

The Smith Chart

Plot

normalized

impedance

zL=1+j2

6

The Smith Chart

7

The Smith Chart • Impedance:

– Z1 = 100 + j50 – Z2 = 75 -j100 – Z3 = j200 – Z4 = 150 – Z5 = infinity (an open circuit) – Z6 = 0 (a short circuit) – Z7 = 50 – Z8 = 184 -j900

• Normalized impedance (line

impedance (50 Ohms) : – z1 = 2 + j – z2 = 1.5 -j2 – z3 = j4 – z4 = 3 – z5 = infinity – z6 = 0 – z7 = 1 – z8 = 3.68 -j18

8

The Smith Chart

•A complete revolution (3600)

around Smith Chart represents

a distance of (λ/2) on the line.

λ distance on the line

corresponds to a 7200

movement on the chart.

λ→ 7200

•Clockwise movement

represents moving toward the

Generator.

•Counter-clockwise movement

represents moving toward the

Load. 9

The Smith Chart

Three scales:

•Outermost scale: distance on

line in terms of wavelength,

moving toward Generator.

•Middle scale: distance on line

in terms of wavelength,

moving toward Load.

•Innermost scale : to

determine θΓ (in degrees)

10

The Smith Chart

Given Z0, ZL, λ and length

of line, We can determine

Zin, Yin, s, and Γ.

11

Example 11.4

•A lossless transmission line with Z0=50 Ω is 30 m long and operates

at 2 MHz. The line is terminated with a load ZL=60+j40 Ω. If u=0.6c

on the line, find

•(a) The reflection coefficient Γ

•(b) The standing wave ratio s

•(c) The input impedance.

0L 0

L 0

Method 1 (Without the Smith Chart)

Z Z 60 40 50 10 40(a) = 0.3523 56

Z +Z 60 40 50 110 40

1 | | 1 0.3523( ) s= 2.088

1 | | 1 0.3523

Solution

j j

j j

b

12

Example 11.4- Solution continued

60

8

00

0

0

0

0

2 (2 10 ) 2(c) = (30) 120 (electrical length)

0.6(3 10 ) 3

tan

tan

60 40 50 tan120 50

50 (60 40) tan120

23.97 1.35 24.01 3.22

Lin

L

l lu

Z jZ lZ Z

Z jZ l

j j

j j

j

0

0

0

(a) :

60 40 =1.2+j0.8

50

Locate at point

0| | 0.3516

0

is between 0 and 0 :

angle 0 56

0.3516 56

_____________________

( ) To find standing wave

ratio , draw s-ci

LL

L

L

L

ZNormalized z

Z

j

z

P

Q

S P

P S

b

s

P

rcle

(radius 0P and center 0)

s-circle meets -axis

at 2.1

r

s

13

Example 11.4

in

8 00

6

0

(c) to find Z , express interms of or in degrees.

0.6(3 10 ) 30 72090 m, =30 m= 240

2 10 90 3 3

Move clockwise from load toward Generator 240 on the

s-circle from point to point . A

l

ul

f

P G

0

t , We obtain: 0.47 0.03

Hence 50(0.47 0.03) 23.5 1.5

in

in in

G z j

Z Z z j j

zL

14

Example 11.5

A load of 100+j150 Ω is connected to a 75 Ω lossless line. Find:

a) The reflection coefficient Γ

b) The standing wave ratio s

c) The load admittance YL

d) Zin at 0.4λ from the load.

e) The locations of Vmax and Vmin with respect to the load if the line

is 0.6 λ long.

f) Zin at the generator.

15

Example 11.5

0

0

0

0

0

0

100 150(a)

75

=1.33+j2 (point )

0| | 0.659

0

angle 0 40

0.659 40

:

100 150 75

100 150 75

0.659 40

____________________

( ) Draw s-circle passing

thro

LL

L

L

LL

L

L

L

Z jz

Z

P

P

Q

P S

Z Z

Z Z

j

C

j

heck

b

chec

ugh

k:

and obtain

s=4.82

1 | | s= 4.865

1 | |

P

16

Example 11.5

0

0 0

0

(c) y 0.228 0.35

y

1 (0.228 0.35)

75

3.04 4.67

:

1 1

100 150

3.07 4.62

( ) The 0.4 corresponds

to 0.4 720 288

Move 288 on s-circle

from toward generator

L

L L

L

L

L

j

Y Y

j

Y j mS

YZ j

j

Che

mS

d

k

P

c

0

(clockwise) to reach point .

0.3 0.63

75(0.3 0.63)

=22.5+j47.25

in

in in

R

z j

Z Z z j

17

Example 11.5 – Solution continued

0

0

00

0

0

0

0

( )

2(0.4 ) 360 (0.4) 144

tan

tan tan

100 150 75 tan144 =75

75 (100 150) tan tan144

=54.41 65.

:

25

Lin

L

in

d

l

Z jZ

C

lZ Z

Z jZ l

j j

j j

or

Z

heck

21.9 47.6 j

18

Example 11.5 0

mi

0

0

0

0

n

(e) 0.6 0.6 720 432

1 72

Start from (Load), move

alone s-circle 432 , or one

revolution +72 , and reach

Generator at point .

We have passed through

point (location of V )

once, and po

P

G

revolution

T

max

max

0

0

max

min

int (location

of ) twice. From load:

1st V is located at :

400.055

720

2nd V is located at :

0.055 0.5552

The only V is located at :

0.0

V

55 / 4 0.3055

S

19

Example 11.5

(f) At (Generator end),

1.8 - 2.2

75(1.8 - 2.2)

135- 165

in

in

G

z j

Z j

j