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Transcript of Example of Final Project Thesis
BEng (Hons) in Electrical & Electronics Engineering 3+0in collaboration with UNIVERSITY OF EAST LONDON.
LOOP PATCH ANTENNA DESIGN
BY ABUBAKAR MAHDI ALHAJI 1
900MHz CIRCULAR LOOP PATCH ANTENNADESIGN AND IMPLEMENTATION
FINAL YEAR PROJECT REPORT
XXX
BACHELOR OF ENGINEERING (HONS)ELECTRICAL & ELECTRONIC
ENGINEERING (COMMUNICATION)
UNIVERSITY OF EAST LONDON
JANUARY 2012
BEng (Hons) in Electrical & Electronics Engineering 3+0in collaboration with UNIVERSITY OF EAST LONDON.
LOOP PATCH ANTENNA DESIGN
BY ABUBAKAR MAHDI ALHAJI 2
900MHz CIRCULAR LOOP PATCH ANTENNA DESIGN ANDIMPLEMENTATION
XXXXX
A project report submitted in partial fulfillment of the requirements for the award ofdegree of Bachelor of Engineering (Hons) in Electrical & Electronic Engineering
(Communication)
UNIVERSITY OF EAST LONDON
JANUARY 2012
DECLARATION
BEng (Hons) in Electrical & Electronics Engineering 3+0in collaboration with UNIVERSITY OF EAST LONDON.
LOOP PATCH ANTENNA DESIGN
BY ABUBAKAR MAHDI ALHAJI 3
I hereby declare that this project entitled " 900MHz CIRCULAR LOOP PATCH
ANTENNA DESIGN AND IMPLEMENTATION" has been done by myself under the
supervision of Mr. ALI ZUHAIR, and no portion of the work contained in this report has
been submitted in support of any application for any other degree of qualification of this
or any other university or institute of higher learning.
I declare that this project is entirely my own work except where due references are
made.
Signature: _______________
Name:
UEL ID:
Date:
Supervisor's Signature: _____________________
Supervisor's name
Date:
BEng (Hons) in Electrical & Electronics Engineering 3+0in collaboration with UNIVERSITY OF EAST LONDON.
LOOP PATCH ANTENNA DESIGN
BY ABUBAKAR MAHDI ALHAJI 4
iiACKNOWLEDGEMENT
Initially, I thank Almighty Allah for making this project a success. This project
mainly was achieved with the help of hard-working people that guide me throughout my
final year project and will also say thanks to those important people who spend time and
being patient while doing this project.
Special appreciation to my project supervisor, Mr. ALI ZUHAIR for his guidance
and advice. He inspired me, used human management skills in order to encourage me,
and shared his ideas during the course of this project. I completed my project and also
got the opportunity to learn and develop skills for myself in the future.
The rest of engineering staffs in Stamford college were very helpful and many of the
expert in antenna research. Next I would like to thank my parents who give financial
support throughout my course.
BEng (Hons) in Electrical & Electronics Engineering 3+0in collaboration with UNIVERSITY OF EAST LONDON.
LOOP PATCH ANTENNA DESIGN
BY ABUBAKAR MAHDI ALHAJI 5
iiiABSTRACT
This project is about the circular loop patch antenna design that operates in 900MHz
frequency. The antenna is a single loop patch which lies on the surface of the dielectric
substances, FR4. A 50 SMA RF port is attached at the end tip of the antenna for 50
coaxial cable connection.
The antenna is designed and simulated using ADS software. The concerned
parameters of the antenna are, S11, Gain and impedance. Apart from these, other concern
parameters are radiation pattern and power also will be take into consideration when
simulate antenna.
At the end of the project, a working loop patch antenna will be demonstrated and
operate at 900MHz. If network analyzer is not available, a television will be used to test
the working of the antenna. By connecting the loop patch antenna to the television, one
channel or more can be received and see clearly.
BEng (Hons) in Electrical & Electronics Engineering 3+0in collaboration with UNIVERSITY OF EAST LONDON.
LOOP PATCH ANTENNA DESIGN
BY ABUBAKAR MAHDI ALHAJI 6
iv
.
TABLE OF CONTENTS
Page
Declaration .......................................................................................................................ii
Acknowledgements...........................................................................................................iii
Abstract.............................................................................................................................iv
Table of Contents..............................................................................................................vi
List of Figures..................................................................................................................vii
List of Abbreviations.......................................................................................................viii
CHAPTER 1: INTRODUCTION.................................................................................1
1.1 Background.........................................................................................................1
1.2 Statement of The Problems.................................................................................2
1.3 Objectives...........................................................................................................3
1.4 Scope of the Project............................................................................................3
1.5 Expected Outcome of the Project.......................................................................4
1.6 Technical proposed block diagram to implement the project.............................5
1.7 Overview of the report........................................................................................6
CHAPTER 2: REVIEW OF LITERATURE..............................................................8
BEng (Hons) in Electrical & Electronics Engineering 3+0in collaboration with UNIVERSITY OF EAST LONDON.
LOOP PATCH ANTENNA DESIGN
BY ABUBAKAR MAHDI ALHAJI 7
2.1 The Theory of Loop Antenna.............................................................................8
2.2 Radiated Fields...................................................................................................10
2.3 Power Density of the Loop Antenna..................................................................13
2.4 Loop Patch Antenna Design...............................................................................13
CHAPTER 3: SYSTEM DESIGN................................................................................16
3.1 Design requirements.............................................................................................19
3.2 Loop Patch Antenna Design.................................................................................19
CHAPTER 4: HARDWARE & SOFTWARE IMPLEMENTATION.....................24
4.1 Hardware Requirement for the making of Loop Patch Antenna.........................24
4.1.1 FR4 PCB Copper Board................................................................................24
4.1.2 SMA Port.......................................................................................................25
4.1.3 SO239 Port.....................................................................................................26
4.1.4 50 Coaxial Cable.........................................................................................27
4.1.5 75 Coaxial cable..........................................................................................28
4.1.6 Soldering Gun................................................................................................29
4.1.7 Soldering Lead ..............................................................................................30
4.2 Software Requirement to design the Loop Patch Antenna..................................31
4.3 Loop Patch Antenna Design using ADS..............................................................31
4.4 The Making of Loop Patch Antenna....................................................................40
CHAPTER 5: RESULTS & DISCUSSIONS..............................................................50
5.1 Simulation Results................................................................................................50
5.2 Experimental Test of Loop Patch Antenna...........................................................64
5.3 Apply and test the Loop Patch Antenna using Television....................................71
5.3.1 The performance of commercial type of loop antenna...................................71
5.3.2 The performance loop patch antenna developed in this project.....................72
BEng (Hons) in Electrical & Electronics Engineering 3+0in collaboration with UNIVERSITY OF EAST LONDON.
LOOP PATCH ANTENNA DESIGN
BY ABUBAKAR MAHDI ALHAJI 8
CHAPTER 6: CONCLUSIONS AND RECOMMENDATIONS..............................75
6.1 Conclusion............................................................................................................75
6.2 Problem Facings...................................................................................................76
6.3 Recommendation.................................................................................................76
REFERENCES..............................................................................................................77
APPENDIX A: RADIO FREQUENCY SPECTRUMS.............................................79
APPENDIX B: INPUT IMPEDANCE OF LOOP ANTENNA GRAPHS...............80
APPENDIX C: LAYOUT OF LOOP PATCH ANTENNA......................................81
APPENDIX D: PRICE LIST.......................................................................................82
APPENDIX E: GANTT CHART................................................................................83
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LOOP PATCH ANTENNA DESIGN
BY ABUBAKAR MAHDI ALHAJI 9
LIST OF FIGURES
Page
Figure 1.1: Application of loop antenna in metal detector................................................2
Figure 1.2: Application of loop antenna in VHF/UHF frequency....................................2
Figure 1.3: The scope of the project..................................................................................3
Figure 1.4: Expected outcome of the project.....................................................................4
Figure 1.5: Technical block diagram to implement the project.........................................5
Figure 2.1: Loop antennas.................................................................................................9
Figure 2.2: Geometry of circular loop..............................................................................10
Figure 2.3: Resistance versus the directivity ................................................................14
Figure 2.4: Reactance versus the directivity .................................................................15
Figure 3.1: A process to build a 900MHz loop patch antenna.........................................16
Figure 3.2: Determine the 50 resistance from the graph..............................................21
Figure 3.3: The physical appearance of the loop patch antenna......................................23
Figure 4.1: FR4 PCB copper board.................................................................................24
Figure 4.2: SMA Port......................................................................................................25
Figure 4.3: SO239 Female port.......................................................................................26
Figure 4.4: 50 Coaxial cable........................................................................................27
Figure 4.5: 75 TV coaxial cable...................................................................................28
Figure 4.6: Soldering gun................................................................................................29
Figure 4.7: Soldering lead...............................................................................................30
Figure 4.8: ADS starting window...................................................................................31
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LOOP PATCH ANTENNA DESIGNBY ABUBAKAR MAHDI ALHAJI
10
Figure 4.9: Creating new project.....................................................................................32
Figure 4.10: New project template window....................................................................32
Figure 4.11: Schematic window......................................................................................33
Figure 4.12: The window for patch antenna design.........................................................34
Figure 4.13: Dimension of the measurement in 2D coordinates system..........................35
Figure 4.14: Important functions to sketch the path loop antenna...................................35
Figure 4.15: Draw a circle in the ADS software..............................................................36
Figure 4.16: Draw a second circle and overlap it.............................................................36
Figure 4.17: Creating a single loop on the circle..............................................................37
Figure 4.18: A ring or a single turn of loop patch antenna...............................................37
Figure 4.19: Strip of conductor joint with the ring...........................................................38
Figure 4.20: Joining the strip and loop together...............................................................39
Figure 4.21: The complete loop patch antenna design.....................................................40
Figure 4.22: Print out the loop patch antenna layout from ADS software.......................41
Figure 4.23: Material prepared for ironing process..........................................................42
Figure 4.24: Use sticker to hold the print out and put on the PCB board........................42
Figure 4.25: Ironing in progress.......................................................................................43
Figure 4.26: The ironing process time phases..................................................................44
Figure 4.27: Result after ironing process and darken the image......................................45
Figure 4.28: Prepare for etching.......................................................................................45
Figure 4.29: Etching in progress......................................................................................47
Figure 4.30: Process of making the loop patch antenna after etching.............................48
Figure 4.31: The final outlook of the circular loop patch antenna...................................49
Figure 4.31: The final outlook of the circular loop patch antenna...................................49
Figure 5.1: Window that allow user key in the antenna parameters.................................50
Figure 5.2: Simulation control window............................................................................51
Figure 5.3: S11 and S22 simulation results of loop patch antenna shown in Figure 4.21..52
Figure 5.4: The meaning of S11 and S22 on the loop patch antenna..................................53
Figure 5.5: The Smith charts plot for S11 and S22.............................................................55
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LOOP PATCH ANTENNA DESIGNBY ABUBAKAR MAHDI ALHAJI
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Figure 5.6: Impedance plot of the loop patch antenna.....................................................56
Figure 5.7: VSWR plot of loop patch antenna.................................................................58
Figure 5.8: Ready to plot the radiation pattern.................................................................59
Figure 5.9: Circular polarization radiation pattern...........................................................60
Figure 5.10: The gain and directivity radiation pattern....................................................61
Figure 5.11: Efficiency of the loop patch antenna............................................................61
Figure 5.12: 3D view of loop patch antenna....................................................................62
Figure 5.13: Three 3D radiation pattern of the loop patch antenna.................................63
Figure 5.14: Network analyzer.........................................................................................64
Figure 5.15: Network analyze test on loop patch antenna................................................65
Figure 5.16: The S11 plot of the loop patch antenna.........................................................66
Figure 5.17: The Smith Chart plot of loop patch antenna................................................68
Figure 5.18: Impedance plot of loop patch antenna.........................................................69
Figure 5.19: The VSWR plot............................................................................................70
Figure 5.20: Using commercial type of loop antenna to receive the TV channels...........71
Figure 5.21: Using loop patch antenna to receive the TV channels.................................72
Figure 5.22: Analysis on how loop patch antenna works to receive the TV channel......73
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LOOP PATCH ANTENNA DESIGNBY ABUBAKAR MAHDI ALHAJI
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LIST OF ABBREVIATIONS
RF - Radio Frequency
PCB - Printed Circuit Board
SMA - Subminiature Version A
UHF - Ultra High Frequency
VHF - Very High Frequency
HF - High Frequency
VSWR - Voltage Standing Wave Ratio
TV - Television
S11 - Input reflection coefficient
S22 - Output reflection coefficient
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LOOP PATCH ANTENNA DESIGNBY ABUBAKAR MAHDI ALHAJI
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LIST OF TABLES
Table 3.1 - The technical parameters and design requirement of the antenna.................19
Table 5.1 - Technical features of the network analyzer...................................................65
Table 5.2 - The performance of commercial type of loop antenna..................................72
Table 5.3 - The performance of loop patch antenna on the TV channels reception.........73
Table 6.1 - Summarized the comparison results between simulation and practical.........75
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LOOP PATCH ANTENNA DESIGNBY ABUBAKAR MAHDI ALHAJI
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CHAPTER 1: INTRODUCTION
1.1 Background
Antenna plays an important role to receive and transmit the RF signal in wireless
communication. The size of antenna varies from one to another and depends on the
operating frequency. The size of antenna usually determine by wavelength.
Today a variety of antennas can be seen everywhere. Generally the antennas can be
classified under three types: elemental antennas, dish antennas and patch antennas.
Elemental types of antennas are the simple type of wires antenna. The design can be a
simple conductor to a complex structure. Dish antennas are using a reflector to reflect
the RF signal and focus the signal at one point. Patch however is a flat antenna or
conductor which can be many shapes and lie on a piece of dielectric material. Many
small wireless electronic communication devices such as cell phones are using patch
antennas.
In this project, a circular loop patch antenna operates at 900MHz frequency is
designed and implemented. The loop patch antenna in this project consists of single loop
of copper conductor lies on FR4 material which having a relative permeability of 4. A
50 SMA port is attached at the end point of the antenna for coaxial cable connection.
At the end of construction of the antenna, the antenna will be send for testing in the RF
lab using network analyzer.
To implement or apply the antenna into real time, the antenna may be tested using
television to observe the channels received.
1.2 Statement of the problems
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LOOP PATCH ANTENNA DESIGNBY ABUBAKAR MAHDI ALHAJI
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Loop patch antenna is not concerned by many RF researchers. This is because its
dimension usually big in size and difficult to implement. In the past ten years [1], many
metal detectors are using loop antennas, but not in patch format, to detect the land mine
or any metal objects burry under the ground. This kind of loop antenna made from many
turns of wires and heavy in weight. Besides that, the operating frequency of the loop
antenna used by the metal detectors are low in frequency. This can be easily distorted by
noise. Figure 1.1 shows typical metal detector [2]:
Figure 1.1 - Application of loop antenna in metal detector [2].
Figure 1.2 - Application of loop antenna in VHF/UHF frequency [3].
Figure 1.2 shows the loop antenna also used for indoor TV channels reception. As
seen in the diagram, the loop is very big in size and inconvenient to install.
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LOOP PATCH ANTENNA DESIGNBY ABUBAKAR MAHDI ALHAJI
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1.3 Objectives
The objective of this project is to:
Design and implement a loop patch antenna that operates at 900MHz.
The gain of the antenna must be greater than 2dBi.
The antenna has to resonance at 900MHz.
The input impedance of the antenna must be 50.
The antenna must at least receive one television channel.
1.4 Scope of the project
The scope of the project is shown in Figure 1.1:
Figure 1.3 - The scope of the project.
As seen in Figure 1.3, the scope of the project covers the design and construction of
the loop path antenna. After design, the parameters will be keyed into antenna
Scope of the project
Design aloop pathantenna
Fabricate theantenna
Simulate theantenna usingADS
Test and analyze theresults
BEng (Hons) in Electrical & Electronics Engineering 3+0in collaboration with UNIVERSITY OF EAST LONDON.
LOOP PATCH ANTENNA DESIGNBY ABUBAKAR MAHDI ALHAJI
17
simulation software (ADS) to compute and optimize the gain as well as the resonance
frequency.
If the result of the simulation is satisfied, next proceed to the fabrication stage. In this
stage, the PCB board which also called FR4 board will be used to make a loop antenna.
Finally, the antenna is sends for testing using network analyzer and applies it to detect
the television channels.
1.5 Expected Outcome of the Project
Figure 1.4 shows the expected outcome of the project:
Figure 1.4 - Expected outcome of the project.
The parts, name and functions of the antenna is summarized into table 1.1.
Parts Name Functions
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LOOP PATCH ANTENNA DESIGNBY ABUBAKAR MAHDI ALHAJI
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56 Loop antenna A copper conductor used to receive the signals34 FR4 dielectric material To support the loop antenna12 50 SMA port Connect to coaxial cable
Table 1.1 - Summarized the parts, name and functions of the loop antenna
1.6 Technical proposed block diagram to implement the project
Figure 1.5 - Technical block diagram to implement the project.
Figure 1.5 shows general view of project components. As seen in the block diagram, the
loop patch antenna developed consists of SMA connector or SO239 connector. The
SMA connector is only used when the antenna tested under network analyzer whereas
the SO239 is used when the antenna is tested using television.
Loop patch antennaSMA or SO239 port
TV/RF signal generator(Optional)
Network analyzer
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In other words, the SMA or SO239 are the ports to fetch the RF signal. Since antenna
is a reciprocal device, it can be work for both transmitting and receiving. As a matter of
fact, to view the transmitting signal and receiving signal, a network analyzer is used. In
this network analyzer, the RF signal is generated internally and transmit to the loop
patch antenna via 50 coaxial cables. The signal is then returned back to network
analyzer using the same cables. From transmit and receive signal, the network analyzer
can determine S11 (input impedance), VSWR and return loss of the antenna.
RF signal generator is an optional source to connect to the antenna for testing. If the
network analyzer does not has RF source function, then RF signal generator is needed.
Television is connected to see whether the loop patch antenna can be used to receive the
VHF/UHF signal or not. This will be shown later in this report.
1.7 Overview of the report
Chapter 1 of this report is an introduction. This chapter introduces overview of the
project and its objectives. The chapter also explains the technical content of the project
in terms of block diagram. Apart from that, chapter 1 highlights the overview of the
report chapters.
Chapter 2 is a literature review. This chapter discusses theory of loop antenna and
design issues. Reviewing the current loop patch antenna research also fall into this
chapter.
Chapter 3 is about the methodology. This chapter will show systematic way to
implement the project. A flow chart is used to summarize the entire work and a detail
explanation on the method used to design the antenna.
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Chapter 4 is hardware and software implementation. This chapter discusses the
components used in the project, how the components combined to made a loop patch
antenna and software used to design and simulate the antenna.
Chapter 5 is a results display and analysis. This chapter mainly discusses the data
collected from the experimental works. The chapter also explains technical issues on the
design of hardware as well as the problem facing.
Chapter 6 is a conclusion chapter. This chapter concludes the project outcomes and
its limitation. Advantages and disadvantages also will be stated in this chapter. Future
improvement on the project will be briefly described in this chapter too.
CHAPTER 2: REVIEW OF LITERATURE
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2.1 The Theory of Loop Antenna
Loop antennas take many different forms such as rectangle, square, triangle, ellipse,
circle and many other configurations. Because of the simplicity in analysis and
construction, the circular loop is the most popular and has received the widest attention.
It will be shown that a small loop is equivalent to an infinitesimal magnetic dipole
whose axis is perpendicular to the plane of the loop. That is, the fields radiated by an
electrically small circular loop are of the same mathematical form as those radiated by
an infinitesimal magnetic dipole [1].
Loop antennas are usually classified into two categories, electrically small and
electrically large. Electrically small antennas are those whose overall length (number of
turns times circumference) is usually less than about one tenth of the a wavelength (NC
< /10). However, electrically large loops are those whose circumference is about a free
space wavelength (C ~ ). Most of the applications of loop antennas are in HF (3 -
30MHz), VHF (30 - 300MHz) and UHF (300 - 3000MHz) bands. When used as field
probes, they find applications even in the microwave frequency range [2].
Loop antennas with electrically small circumference or perimeters have small
radiation resistances that are usually smaller than their loss resistances. Thus they are
very poor radiators, and they are seldom employed for transmission in radio
communication. When they are used in any such application, it is usually in the
receiving mode, such as in portable radios and pagers, where antenna efficiency is not as
important as the signal to noise ratio. They are also used as probes for field
measurements and as directional antennas for radio wave navigation. Figure 2.1 shows
few examples of existing loop antennas.
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Figure 2.1 - Loop antennas [3].
The field pattern of electrically small loop antennas is similar to that of an infinitesimal
dipole with a null perpendicular to the plane of the loop and with its maximum along the
plane of the loop. As the overall length of the loop increases and its circumference
approaches one free space wavelength, the maximum of the pattern shifts from the plane
of the loop to the axis of the loop which is perpendicular to its plane [4].
The radiation resistance of the loop can be increased and made comparable to the
characteristic impedance of practical transmission lines, by increasing its perimeter or
the number of turns. Another way to increase the radiation resistance of the loop is to
insert within its circumference or perimeter, a ferrite core of very high permeability
which will raise the magnetic field intensity and hence the radiation resistance. This
forms so called ferrite loop.
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2.2 Radiated Fields
To find the fields radiated by the loop, we need to consider the potential function in
three dimensional spaces. This is given by [5]:
4)z,y,x(A
C
This equation can be derived by referring to Figure 2.2 [6]:
From Figure 2.2, R is the distance from any point on the loop to the observation
point and dl' is an infinitesimal section of the loop antenna. In general, the current
distribution Ie(x', y', z') can be writte
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LOOP PATCH ANTENNA DESIGNMAHDI ALHAJI
To find the fields radiated by the loop, we need to consider the potential function in
three dimensional spaces. This is given by [5]:
'dR
e)'z,'y,'x(I
jkR
C
e
This equation can be derived by referring to Figure 2.2 [6]:
Figure 2.2 - Geometry of circular loop [6].
From Figure 2.2, R is the distance from any point on the loop to the observation
is an infinitesimal section of the loop antenna. In general, the current
(x', y', z') can be written as:
To find the fields radiated by the loop, we need to consider the potential function in
(1)
eometry of circular loop [6].
From Figure 2.2, R is the distance from any point on the loop to the observation
is an infinitesimal section of the loop antenna. In general, the current
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Ie(x', y', z') = ax Ix(x', y', z') + ay Iy(x', y', z') + azIz(x', y', z')
(2)
For the circular loop antenna shown in Figure 2.2, it would be more convenient to write
the rectangular current components in terms of the cylindrical components using matrix
as [7]:
zz
y
x
I
I
I
100
0'cos'sin
0'sin'cos
I
I
I
(3)
For the circular loop, the current is flowing in the direction so that [8]:
Ie = arIsinsin(-') + aIcos sin(-') + aI cos(-')
(4)
The distance R, from any point on the loop to the observation point, can be written as
[9]:
222 )'zz()'yy()'xx(R
(5)
Since
x = r sincos
y = r sinsin
z = r cos
x' = a cos'
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y' = a sin'
z' = 0
The equation 5 can be reduced to [10]:
)'cos(sinar2arR 22 (6)
The differential element length is given by [10]:
dl' = a d' (7)
Hence equation 1 can be simplified to [10]:
'd'cossinar2ar
e'cos
4
IaA
22
'cossinar2arjk2
0
0
22
(8)
Using Maclaurin series to simplify the integration and introducing H and E as magnetic
field and electric field components, the magnetic field reduced to [11]:
jkr
2
02
r ejkr
11
r2
cosIkajH
(9)
jkr
2
02
e)kr(
1
jkr
11
r4
sinI)ka(H
(10)
The electric fields correspond to [12]:
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Er = E = 0
E = jkr02
ejkr
11
r4
sinI)ka(
(11)
2.3 Power Density of the Loop Antenna
The fields radiated by a small loop are valid every where except at the origin. The
power in the region very close to the antenna is predominantly reactive and in the far
field is predominantly real. To illustrate this, the complex power density is defined as
[13]:
)HE(2
1W (12)
When equation 12 is integrated over a closed sphere, only its radial component given by:
32
22
0
4
r)kr(
1j1
r
sin|I|
32
)ka(W (13)
Which contribute to the complex power Pr. Thus [13]:
ddsin)kr(
1j1|I|
32
)ka(dsWP 3
2
0
2
03
20
4
r (14)
Which reduces to:
3
20
4r
)kr(
1j1|I|)ka(
12P (15)
2.4 Loop Patch Antenna Design
The loop patch antenna design is begin by considering the size. This can be done
using the equation shown below [14]:
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f
c (16)
Where is a wavelength express in meter.
Once the size of the loop is determined, it is then proceed to calculate radius of the loop.
This can be obtained using equation 17 [15].
2r a
3
2120R
(17)
Where Rr is a characteristic impedance 50 and "a" is a radius of the loop antenna.
The gain and directivity of the antennas can be obtained from the chart as shown in
Figure 2.3 and 2.4.
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Figure 2.3 - Resistance versus the directivity [16].
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Figure 2.4 - Reactance versus the directivity [16].
The conductor length connected to the loop antenna and the port is normally given by
/4 long. If there is a spacing happen due to two conductors lengths are used, then the
spacing equation is given by [17]:
1
2
f2
cS
r (18)
Where S = Spacing
f = frequency
c = speed of light
r = dielectric constant
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CHAPTER 3: SYSTEM DESIGN
Project design steps are very important to achieve the objectives. A successful project
is because of proper planning and implementation. This chapter will shows a detail of
system design of the project. The general design of the loop patch antenna can be
summarized as shown in Figure 3.1.
Yes No
Figure 3.1 - A process to build a 900MHz loop patch antenna.
Study the looppatch antennaparameters
Highlight the designrequirements
Manually design the antenna todetermine its dimension based on thefrequency and gain requirement.
Put all the design parameters into antennasimulation software
Test and analyze the results
Fabricate the antenna
Changeparameters
Is the simulationresult correct?
Simulate the antenna
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The first step of designing the project is to identify the parameters of the loop patch
antenna and the antenna features. The study of loop patch antenna or the information
regarding the antennas can be obtained from the following resources:
Internet
Journals
Conference papers
Antenna textbooks
Among all the resources, textbooks will be widely used compared to others. The antenna
books provide sufficient information on the design of loop patch antenna. Not only that,
the book also contents the detail design of the antenna.
Journal and conference papers are used as a guideline in implementing the loop patch
antenna. Journal and conference papers do not provide clear or detail in the system
design of the antenna. As a matter of fact, these two resources normally used to
determine the similar works or research that has been done by some one else. They also
used for comparison purposes.
Internet is a huge library. Internet can provide information on the loop patch antenna
designs. However, this does not mean that the text in the literature review is copy from
internet. In this project, the use of internet is to fetch some picture information, not the
text information. Lecturers and examiners are welcome to upload this document to
"Turn-It-In" plagiarism checker to check for plagiarism.
After getting enough information on the loop patch antennas. It is then perform
manual design on the antenna. Of course, the design requirement must be highlighted
before the simulation. The design requirement will be shown in next section.
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Once the antenna has been manually design on a piece of paper, the parameters are
then keyed into the antenna simulation software. Although there are many antenna
simulation software available in the market, however, the ADS (Advanced Design
System) antenna simulation software will be used. This software is developed by Agilent
company in 2002. A pirated version of this software can get from many computer shops.
The advantages of using ADS are:
1. Automatic scale the antenna size once the parameter such as permeability and
dielectric constant as well as the frequency values has been keyed in.
2. Fast computation using mesh integration and green theorem.
3. The results can be optimized until desire results are obtained.
4. For the antenna design, the simulation results will show: radiation pattern in 2D/3D,
power transmit/receive, S-parameters, Smith chart, gain, impedance and directivity
plots.
Simulation usually will take longer times because of optimization to get a better
result. For example, the loop patch antenna in this project is operates in 900MHz.
However, this does not mean that after manually design and key in those parameters into
the ADS software, the result will directly show resonance at 900MHz. In the real time,
the results get from the first simulation will be different from the expected results. As a
matter of fact, optimization is needed.
When the antenna simulation results are all correctly, the next step is proceed to the
antenna fabrication. Fabrication of antenna will be shown detail later in this chapter.
Finally the antenna will be tested in the lab using network analyzer and television.
The results are then compared to the simulation results.
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3.1 Design requirements
This section will shows the loop patch antenna technical design requirements. The
requirements are listed and stated in table 3.1.
Parameters RequirementsFrequency 900MHzGain > 2dBiRadiation pattern CircularInput impedance, S11 50VSWR 1 - 3No. of turns of the loop 1Shape of the loop Circular
Table 3.1 - The technical parameters and design requirement of the antenna.
3.2 Loop Patch Antenna Design
Step1: Determine the overall size of the antenna
To determine the overall size of the antenna, the design must begin with frequency and
calculate the wavelength. Wavelength is the only parameter that can tell the overall size
of the antenna. Hence, for the loop patch antenna operate in 900MHz,
Size of antenna:6
8
10900
103
f
c
= 33.3cm
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Step 2: Find the radius of the loop
Since the RF source having is 50 of output impedance, we are expecting radiation
resistance to be 50 as well as so that maximum power can be transfer. With that, we
can find out the radius of the loop.
2r a
3
2120R
2a3
212050
a = 0.25m or 25cm
Hence, the radius of the loop is 25cm.
The circumference is = 2r = 20.25 = 1.57m or 157cm
Step 3: Find the circumference of the loop
To find out the circumference of the circular loop, it is important to refer the graph
shown in Figure 3.2 (resistance graph). Since only = 8 can give lower resistance
which is nearly 50, then from the graph in Figure 3.2, ka = c/ is 0.3.
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Figure 3.2 - Determine the 50 resistance from the graph.
So, the second loop which has circumference of:
0.30.333 = 0.0999m or 9.99cm
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Step 4: Determine the length which strip conductor that connect to the loop.
The length connecting loop in the form of patch is determine using /4. So, the length is:
/4 = 33.3/4 = 8.235cm
Step 5: Calculate the width of the strip conductor.
The width of the conductor that connects to the loop is then given by:
W = L/10 = 8.235cm./10
= 0.8235cm
Step 6: Calculate the conductor separation.
Since two equal size of conductors are used and connected to the loop, then a suitable
spacing is:
1
2
f2
cS
r
Where r dielectric constant of the material to build the loop antenna.
C is speed of light.
So, the spacing is:
144
2
109002
103S
6
8
= 0.035m = 3.5cm
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Where 44 is a dielectric constant of FR4 board which is used to make the loop antenna.
Step 7: Sketch the diagram of the design.
Based on the calculated parameters, the outcome or physical appearances of the loop is
then sketch and shows in Figure 3.3.
Figure 3.3 - The physical appearance of the loop patch antenna.
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CHAPTER 4: HARDWARE & SOFTWARE IMPLEMENTATION
This chapter shows the hardware and software implementation of the project. The
chapter will begin by introducing the hardware components needed to build the loop
patch antenna and then followed by software ADS.
4.1 Hardware Requirement for the making of Loop Patch Antenna
The hardware requires used to build antenna is FR4 PCB copper board, SMA port,
SO239 port, 50 coaxial cable, soldering gun and soldering lead. Each of the
components will be briefly describe in this section.
4.1.1 FR4 PCB Copper Board
Figure 4.1 - FR4 PCB copper board.
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FR4 copper board also known as PCB and is a common board to make a circuit for
electronic and electrical. This board can support the signal up to 3GHz. As a result, it is
suitable used to make a patch antenna or printed circuit board antenna. The FR4 is in
single layer of copper. Although double layer also exist, but it cannot be used for the
project because if both sides are conductor, a leak of electromagnetic wave may occurs.
4.1.2 SMA Port
Figure 4.2 - SMA Port.
It is an RF female port which supports the coaxial cable. This port has characteristic
impedance of 50. The port offer excellent electrical performance from DC to 18GHz.
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4.1.3 SO239 Port
This port supports UHF and VHF signals. Typical port is suitable for TV connection.
The port exists in male and female type. The characteristic impedance of the port is 75
As a result, when using this port for loop pat
must be 75 types.
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Figure 4.3 - SO239 Female port.
This port supports UHF and VHF signals. Typical port is suitable for TV connection.
The port exists in male and female type. The characteristic impedance of the port is 75
As a result, when using this port for loop patch antenna connection, typical coaxial cable
This port supports UHF and VHF signals. Typical port is suitable for TV connection.
The port exists in male and female type. The characteristic impedance of the port is 75.
ch antenna connection, typical coaxial cable
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4.1.4 50 Coaxial Cable
Figure 4.4 - 50 Coaxial cable.
The cable is suitable for most of the lab equipments connection such as network
analyzer, function generator or even the spectrum analyzer. The impedance of the cable
would not change as the frequency is change. As a result, this type of cable is very
suitable used for connection between loop patch antenna and the network analyzer for
testing.
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4.1.5 75 Coaxial cable
Figure 4.5 - 75 TV coaxial cable.
The 75 coaxial can be seen every where for those who have television at home. The
cable is only suitable for television to aerial connection. This kind of cable is very
flexible and can stand for weather changed. The cable is also tough and not easy to cut.
As seen in Figure 4.5, the cable has two conductors. One at the center is called core
conductor, which usually connect to positive terminal where as the one at the size is
called secondary conductor for ground connection. The cable only supports VHF to
UHF signals. The impedance of 75 would not change over the range from VHF to
UHF.
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4.1.6 Soldering Gun
Figure 4.6 - Soldering gun.
Soldering gun comes in variety power output. The smallest output power is 18W. The
highest output power is 200W. Soldering gun is used to melt the soldering lead so that
the lead can make connection between SMA port or SO239 port with the loop patch
antenna. Most of the soldering gun works for more than 1A of current with 240V AC
input voltage.
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4.1.7 Soldering Lead
Figure 4.7 - Soldering lead.
Soldering lead melt when expose to high temperature. About 75C, the lead can melt and
becomes solid again when the heat is release. The lead can form of conductor and
usually used for soldering purposes. In the project, the soldering lead is used joint the RF
connector and the loop patch antenna.
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4.2 Software Requirement to design the Loop Patch Antenna
As mentioned before, ADS is a software used to design and simulate the loop patch
antenna. This section will briefly introduce the Agilent ADS software.
4.3 Loop Patch Antenna Design using ADS
The ADS stand for Advance Design System. It is a fasts and accurate patch antenna
simulation software. Figure 4.8 shows the window template to begin the ADS when a
copy of ADS software is available in the computer.
Figure 4.8 - ADS starting window.
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To use the software design any patch antenna, it is always begins with new project.
Figure 4.9 shows the way to click on "New Project".
Figure 4.9 - Creating new project.
Figure 4.10 - New project template window.
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When click on the "New Project", the template window shown in Figure 4.10 will pop
out. In this window, user is asked to key in the project name and unit. The default unit is
in mm. Click "Ok" and the window of Figure 4.11 will appear.
Figure 4.11 - Schematic window.
Note that, the window appears is not the window for the patch antenna design. The
window shows in Figure 4.11 is to design the antenna schematic diagram and it will not
be used in the project.
To go to the window for patch loop antenna design, from Figure 4.11, click
"Window" "Layout" and immediately the window of Figure 4.12 will appear.
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Figure 4.12 - The window for patch antenna design.
There are few important functions in the window of Figure 4.12 to design the loop parch
antenna. Just before shows the functions, user has to take note on the dimension and its
units. Figure 4.13 shows the dimensions in x and y coordinates. Moving the mouse
pointer around will change the dimension values.
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Figure 4.13 - Dimension of the measurement in 2D coordinates system.
To begin design the loop patch antenna, user has to use the function as shown in Figure
4.14:
Figure 4.14 - Important functions to sketch the path loop antenna.
The circle shape shown in Figure 4.14 is used to sketch the circle in order to form a loop.
By following the calculation, the radius of the circle is, 250mm or 25cm, then a click on
the circle shown in Figure 4.14 to draw a circle with radius of 250mm. This is shown in
Figure 4.15.
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Figure 4.15 - Draw a circle in the ADS software.
To create a loop, user has to create another circle which is smaller the one show in
Figure 4.15 then overlap it. This is shown in Figure 4.16.
Figure 4.16 - Draw a second circle and overlap it.
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Now, go to "Edit" "Merge" "Union Minus Intersection" and click on it as seen in
Figure 4.17, the result of circle is then loop like the one show in Figure 4.18.
Figure 4.17 - Creating a single loop on the circle.
Figure 4.18 - A ring or a single turn of loop patch antenna.
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Now, the loop shown in Figure 4.18 needs to connect to the strip of conductor for RF
port insertion. To do that, use the rectangular function shows in Figure 4.14 and create a
connection between strip and the loop. The length should follow the calculated value.
Figure 4.19 shows this.
Figure 4.19 - Strip of conductor joint with the ring.
Notice that when user tries to joint the strip and the loop together, it does not mean that
it is actually jointed together. ADS will not have this automatic jointing the path. As a
matter of fact, to joint the loop and the strip of the conductor, user has to highlight the
two components as shown in Figure 4.20.
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Figure 4.20 - Joining the strip and loop together.
After highlight the two components, then go to "Edit" "Merge" and click on "Union"
to finish the job on joining the components.
The loop patch antenna shown in Figure 4.20 needs to be trimmed and corrected
before doing the simulation. Figure 4.21 shows the final outlook or actual loop patch
antenna that will be used in the project.
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Figure 4.21 - The complete loop patch antenna design.
4.4 The Making of Loop Patch Antenna
This section will show the how the prototype of the loop patch antenna will be made.
The loop patch antenna only can be made when the simulation results are confirmed
correct. If not, it will affect the practical results and hence affect the television channel
receptions.
To build the prototype of loop patch antenna, it important to prepare the materials:
Laser printer, PCB pen, Ironing, A4 size transparent paper, sticker, Iron (III) Chloride,
alcohol solution and clean water.
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The first step of doing the loop patch antenna is print out the antenna layout using
laser printer and A4 size transparent paper as shown in Figure 4.22:
Figure 4.22 - Print out the loop patch antenna layout from ADS software.
After print out, the next step is prepares the FR4 PCB board, PCB pen, sticker and
ironing. This is shown in Figure 4.23. The process of ironing will begin and it is a
process to transfer the image of print out on to the PCB FR4 board. Figure 4.24 shows
the image put on the PCB FR4 board and ready to do the ironing process.
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Figure 4.23 - Material prepared for ironing process.
Figure 4.24 - Use sticker to hold the print out and put on the PCB board.
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The ironing process now begins and it is shown in Figure 4.25.
Figure 4.25 - Ironing in progress.
In the ironing process, heat plays an important role to determine the yield or quality of
image transfer. For good ironing process, the time spends should in between within 10
seconds for temperature of 80C. Figure 4.26 shows the time recorded graph while
ironing is in progress.
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Figure 4.26 - The ironing process time phases.
As seen from the graph shown in Figure 4.26, the total time taken is 80 seconds to do
the whole ironing process. When temperature reaches 80C, the toner transfer will be
started. This takes about 10 seconds.
Figure 4.27 shows the results of image after ironing. Notice that the image of loop
patch antenna has been printed on the FR4 PCB board. If the image printed on FR4
material is not clear. It can be make clearer by using the PCB pen. This is shown in
Figure 4.27 (b).
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(a) Layout printed on FR4 PCB. (b) Darken the image using PCB pen.
Figure 4.27 - Result after ironing process and darken the image.
Figure 4.28 - Prepare for etching.
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Figure 4.28 shows the materials prepare for etching after darken the antenna on the
FR4. Etching is a process that removes materials from such us unwanted copper from
the PCB surface to achieve circuit design requirements. The etching process used in this
project is called chemical etch or pattern etch.
The most important thing about etching is the etch rate. Etch rate will determine the
quality of PCB. Too much etching will remove part of the wanted copper area whereas
little etched will take long time end the process. Hence, etch rate is defined as:
TimeEtch
etchaftercopperofThickness-etchbeforecopperofThichnessrateEtch
The etch time usually affected by few factors as shown below:
The concentration of iron (III) chloride
The temperature
Disturbance of solution
The concentration of iron (III) chloride will determine rate of chemical reaction. In
this etching process, the chemical reaction involve in the etch process is:
FeCl3 + Cu FeCl2 + CuCl
Where FeCl3 is the iron (III) chloride, Cu is copper, FeCl2 is iron (II) chloride and CuCl
is a copper chloride. The rate of reaction is given by:
TakenTime
reactedPCBoncopperofmassTotalreactionofRate
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Figure 4.29 shows the etching in progress and Figure 4.30 shows process of cleaning the
loop patch antenna after etching and attaching the RF port on it.
Figure 4.29 - Etching in progress.
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(a) Clean the antenna after etching. (b) Clean the antenna using alcohol.
(c) Result of loop patch antenna after clean. (d) Solder the SMA port on the tip of the
antenna.
Figure 4.30 - Process of making the loop patch antenna after etching.
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Figure 4.31 - The final outlook of the circular loop patch antenna.
Figure 4.31 shows the complete outlook of the circular loop patch antenna and ready to
go for testing.
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CHAPTER 5: RESULTS & DISCUSSIONS
This section will present the results from the experimental test and practical application
of the loop patch antenna. The discussion will begin with the simulation results followed
by lab test on the loop patch antenna and finally apply the loop patch antenna to receive
the TV channels.
5.1 Simulation Results
To simulate the antenna shown in Figure 4.21, one must go to "Momentum"
"Substrate" and click on "Create/Modify", the window of Figure 5.1 will pop out:
Figure 5.1 - Window that allow user key in the antenna parameters.
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Note that the important parameters that can affect the results of S11, radiation pattern,
input impedance and gain of the antenna are thickness, permittivity and real.
Some parameters cannot changes because it has to follow the practical value. The
parameters such as real and permittivity cannot changes. In real time, the permittivity
and real has to put 40 because the FR4 material used to make the antenna has a
permittivity of 40. The only parameter can change is the thickness of the substrate. In the
market, there are many types of thickness of the substrates. As a result, to tune the
antenna so that it produces desire result, the thickness is one of the concerned parameter
besides side of the antenna or the radius of the antenna.
After key in the antenna parameters, user now has to insert the port at the tip of the
antenna. This port can be clicked from . Without the port, ADS cannot do the
simulation because port is a RF source where it determine the input power.
After inserting the port, user now can go to "Momentum" "Simulation" and click
on "S-parameters". The window of Figure 5.2 will come out.
Figure 5.2 - Simulation control window.
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Figure 5.2 is a simulation control window. As seen in the window, it asks the user to
enter the start frequency and stop frequency. Since the loop patch antenna is operates in
900MHz, a wide range frequency should be entered. From the window, 500MHz to
2GHz is sufficient ranges.
The sample point limit is the amount of iteration. It determines the number of samples
so that a graph can be plotted. The higher the sample point limits, the more accurate the
results but computation will become slow.
After determine the sample point limits and enter the start and stop frequency, it is
then click on "Update" "Apply" "Simulate". The simulation should begin and the
results of S-parameters will automatically plot in the graphs.
Figure 5.3 - S11 and S22 simulation results of loop patch antenna shown in Figure 4.21.
52
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Analysis: Figure 5.4 shows the input reflection coefficient (S11) and output reflection
coefficient (S22) plots of the loop patch antenna. The meaning of S11 and S22 are shown in
Figure 5.4 based on the loop patch antenna design.
Figure 5.4 - The meaning of S11 and S22 on the loop patch antenna.
From Figure 5.3, the S11 is -27.071dB resonance at almost 900MHz. Here the resonance
frequency is 957MHz. The exact 900MHz would not give an expected magnitude of S11.
Basically, the lower the S11 values toward more negative, the better the result is. This is
because it approaches 50 which can match with the impedance of the RF generator.
From Figure 5.3 the S11 = -27.071dB, the input impedance is [18]:
NB: The most important parameters are S11 and S22, because both can transmit and
receive. As for the S12 and S21 they can only receive without transmitting and
transmitting without receiving respectively. Since the antenna is a reciprocal antenna,
then we can only focus on parameters that have reciprocal functions (i.e transmitting
and receiving).
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-27.071dB = 20log10 S11
20
071.27
10
= S11
S11 = 0.0443
50Z
50ZS
in
in11
0.0443 (Zin + 50) = Zin - 50
0.0443Zin + 500.0443 = Zin - 50
0.0443Zin + 2.215 = Zin - 50
2.215 + 50 = Zin - 0.0443Zin
52.215 = 0.9557Zin
9557.0
215.52Z in
= 54.64
Which is very near to 50. Since the ADS using 1Vrms RF signal as a source to obtain
the S11 and S22 parameters, then the transmit power at the output of the RF source is:
Pin(Source) = I2R
= 12 50
= 50W
Since the input and out of the antenna is having the same impedance as 54.64, then the
power that will be radiated by the antenna is:
POut(radiate) = 1254.64
= 54.64W
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The loss of power due to impedance mismatch is:
Power loss = 54.64W - 50W
= 4.64W
Apart from the S11 and S22 graphs plotted, The Smith charts results also shown for S11
and S22. The two Smith charts results are shown in Figure 5.5.
Figure 5.5 - The Smith charts plot for S11 and S22.
Analysis: Looking into the Smith chart and identify the frequency of 957MHz, it is seen
that the loop patch antenna having a complex impedance of 1.045 + j0.01. The actual
impedance is then:
Zactual = 50 (1.045 + j0.01)
= 52.25 + j0.5
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Since the both the circles are toward left, that means the impedance of the loop patch
antenna from 500MHz to 2GHz would be small and typical values is less than 60. The
circles are covered the semi circle of Smith chart on top and bottom. As a result, this can
conclude that the loop patch antenna is having equal inductive reactance and capacitive
reactance. Hence it will be easy to tune to the resonance when construct it in the
practical.
Figure 5.6 shows the impedance plot of the loop patch antenna from 500MHz to
900MHz. Putting the market at near to 900MHz, it shows the impedance is 0.906
normalizes impedance.
Figure 5.6 - Impedance plot of the loop patch antenna.
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Analysis: The graph shows in Figure 5.6 is an impedance plot for the loop patch
antenna from 500MHz to 2GHz. The impedance is given by:
Z = (R jX)
Where Z = Impedance
R = Resistance in real
X = Reactance either capacitance or inductance
We know that X is given by [19]:
fL2XL
fC2
1XC
Hence the Xc or XL are varies with the frequency. That is why we get difference
impedance at difference frequency. Since our concerned frequency is 900MHz, from the
graph, it gives 0.906 normalize impedance. 0.906 is not actual impedance. It is called
normalized impedance by characteristic impedance which is 50. To calculate the
actual impedance, we have to multiply by 50. Hence, actual impedance at 898.4MHz
is:
Zactual = 500.906
= 45.3
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Figure 5.7 shows the VSWR plot of loop patch antenna from the simulation result.
Figure 5.7 - VSWR plot of loop patch antenna.
Analysis: VSWR is a measure of how much the wave is returned to the source when
impedance is mismatched. The practical excepted range of value is from 0 to 2. When
VSWR is more than 2, the antenna is lost its impedance mismatched and it might not be
able to receive any channel. There is a relationship between VSWR and the S11. The
relationship between them can be expressed mathematically as shown below:
11
11
S1
S1VSWR
Since the VSWR = 1.16 at 900MHz,
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1.16 (1 - S11) = 1 + S11
1.16 - 1.16S11 = 1 + S11
1.16 - 1 = S11 + 1.16S11
0.16 = 2.16S11
S11 = 0.074
Convert to dB, we have:
S11(dB) = 20log100.074
= -22.615dB
To plot the radiation pattern of the antenna, user can co go to "Momentum" "Post
Processing" and click on "Radiation pattern". The following window will pop out:
Figure 5.8 - Ready to plot the radiation pattern.
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Analysis: Figure 5.8 shows the window which ready to plot the radiation pattern of the
loop patch antenna. Before plot the radiation pattern, the window request user to select
which types of radiation to be plotted, 2D or 3D? Before looking the 3D, we would like
to see the 2D plot. As a result, use mouse to click on "2D data display". The window also
asks for port excitations, user can choose either one because they are the same. Once
complete setting, click on "Apply" then "Compute". The 2D radiation plot is shown in
Figure 5.9 and 5.10.
Figure 5.9 - Circular polarization radiation pattern.
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Figure 5.10 - The gain and directivity radiation pattern.
Figure 5.11 - Efficiency of the loop patch antenna.
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Although there are many graphs plotted in the radiation 2D radiation patterns. Only
three graphs like circular polarization, gain & directivity and efficiency of the antenna
are useful to describe the performance of loop patch antenna.
From Figure 5.9, it is seen that the radiation pattern of the loop patch antenna is
circular. The red colour represent magnetic field whereas the blue colour is electric
field. Note that both are radiate in the same direction with the same power. As a result,
it can be predict that these fields must be a near field radiation.
Figure 5.10 shows gain and directivity of the loop patch antenna. Notice that the gain
and directivity are having the peak value of 5dB at the angle of 0. Figure 5.11 shows
the efficiency of the antenna. The efficiency of the loop patch antenna is very high which
is about 85%. This shows that only 15% of the power has been loss when operate at
957MHz of frequency.
To view the radiation plot in 3D as well as the prototype of the loop patch antenna in
3D, user has to go back to Figure 5.6 and click on "3D Visualization". The windows of
Figure 5.12 and 5.13 immediately will come out.
Figure 5.12 - 3D view of loop patch antenna.
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Figure 5.13 - Three 3D radiation pattern of the loop patch antenna.
Analysis: Figure 5.12 shows the 3D view of the loop patch antenna with the current
distribution along the loop antenna. The current represented by blue colour and excited
from the port with a little green colour. This indicates the source is from the port.
Figure 5.13 shows the 3D radiation pattern of the loop patch antenna. The radiation
is plotted in the polar coordinate which circulates in 360. The radiation is in circular
polarization as shown.
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5.2 Experimental Test of Loop Patch Antenna
This section presents an experimental test of loop patch antenna in the lab using
network analyzer. Figure 5.14 shows the typical network analyzer used to test the loop
patch antenna:
Figure 5.14 - Network analyzer.
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Table 5.1 shows the technical features of the network analyzer.
Technical Features RequirementPower supply 240V, 50HzMaximum current 20Aone Keypad 4x3No. of ports 2No. of USB port 1Frequency sweep 9kHz - 13.6GHzWindow XpNo. Markers 3Functions Measures S-parameters, Smith chart, impedance, VSWR,
and power transmit/receiveFrequency entered Start, Centre and stopAttenuation 0dB - 50dB
Table 5.1 - Technical features of the network analyzer.
Figure 5.15 shows the loop patch antenna is connected to network analyzer for testing.
Figure 5.15 - Network analyze test on loop patch antenna.
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Figure 5.16, 5.17, 5.18 and 5.19 shows the S11 measurement, Smith chart plot,
impedance plot and VSWR plot
Figure 5.16 - The S11 plot of the loop patch antenna.
Analysis: Figure 5.16 shows the S11 results obtained from the real time network
analyzer machine. Notice that there are quite a number of resonance points happen at
different frequency. However, the most concerned frequency is the one near to 900MHz
because the antenna is operates at 900MHz. From Figure 5.14, the highest peak of S11 is
-24.622dB which happens at 840.16392MHz frequency. This is the only frequency very
to 900MHz. The exact 900MHz would not get resonance due to following factors:
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1. The soldering point between antenna and the port causes resonance point shifted.
2. The N-connector which converts from SMA to network analyzer port causes about -
3dB loss of signal. As a result, this also affects the resonance point of frequency.
From Figure 5.16, the input reflection coefficient S11 at 840.16392MHz is:
- 24.622dB = 20log10S11
20
622.24
11 10S
= 0.0587
0.0587 (Zin + 50) = Zin - 50
0.0587Zin + 2.94 = Zin - 50
2.94 + 50 = Zin - 0.0587Zin
52.94 = 0.9413Zin
9413.0
94.52Z in
= 56.24
Compare to simulation result, we have 54.64. As a matter of fact, the simulation is of
S11 is almost match with the practical result of S11 with almost the same impedance.
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Figure 5.17 - The Smith Chart plot of loop patch antenna.
Analysis: Figure 5.17 shows the Smith chart plot of loop patch antenna. Note that from
the marker point, the impedance shows 57.440 + j15.552 at 841.12671MHz. Compare
to simulation result, it shows 52.25 + j0.5. That means, the practical of loop patch
antenna is more inductive.
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Figure 5.18 - Impedance plot of loop patch antenna.
Analysis: Figure 5.18 shows the impedance plot of loop patch antenna. The impedance
varies with the frequency. At 837.38MHz which is very near to 900MHz, the impedance
is 63.346. Basically the impedance should be the same with calculated which is
56.24. This is because the marker of the network analyzer did not allow positioned to
the frequency of 840.16392MHz. It is too narrow, as a result, the marker only stop at
837.38MHz. Compare with simulation result, the impedance at near the 900MHz is
45.3.
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Figure 5.19 - The VSWR plot.
Analysis: Figure 5.19 shows the VSWR plot of the loop patch antenna tested with
network analyzer. Looking into the graph, the VSWR is 1.385 at the frequency of
839.44MHz. The S11 can be calculated:
11
11
S1
S1VSWR
1.385 (1 - S11) = 1 + S11
1.385 - 1.385S11 = 1 + S11
0.385 = 2.385S11
S11 = 0.1614
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5.3 Apply and test the Loop Patch Antenna using Television
This section will present the application of loop patch antenna to test the TV signal
reception. Since the 900MHz is under the range of VHF/UHF, the antenna should be
able to receive some channels from the Television broadcast station. A comparison
between commercial types of loop antenna with loop patch antenna developed in this
project will be shown.
5.3.1 The performance of commercial type of loop antenna
Figure 5.20 - Using commercial type of loop antenna to receive the TV channels.
Analysis: The commercial type of loop antenna is an elemental type of loop antenna
which using wires to form a loop antenna. In the picture of Figure 5.20, the loop
antenna has two turns. As seen in the pictures, the loop antenna tried to receive the TV
channels from the TV broadcast station. The location of doing the experimental is in
Sunway, Condominium, 5th floor face to North direction and the time is 8pm.
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Table 5.2 shows the results recorded when using the commercial type of loop antenna to
the detect the TV channels in Malaysia.
Available Free TV Channels in Malaysia Detected by commercial type of loopantenna
TV1 TV2 Not clearTV3 NTV7 Not clearTV8 TV9
Legend:
= Able to receive with clear pictures and voice
= Not able to receive and no voice at all
Table 5.2 - The performance of commercial type of loop antenna.
5.3.2 The performance loop patch antenna developed in this project
Figure 5.21 - Using loop patch antenna to receive the TV channels.
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Analysis: Figure 5.21 shows the pictures of using the loop patch antenna receive some
TV channels. As seen in the pictures, by using the loop patch antenna, a much clearly
channels can be received compared to the commercial type of loop antenna. Table 5.3
shows the performance of loop patch antenna on the detection of the TV channels.
Available Free TV Channels in Malaysia Detected by the developed type of loopantenna
TV1 TV2 TV3 Not clearNTV7 TV8 TV9
Table 5.3 - The performance of loop patch antenna on the TV channels reception.
To understand how the loop patch antenna works on receiving the TV channel, one have
to refer to the Gauss's law and Amperes law on current induce when a conductor is
immersed in the electric field.
Figure 5.22 shows the loop patch antenna immersed in the electric field E which
represent the TV channels.
Figure 5.22 - Analysis on how loop patch antenna works to receive the TV channel.
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Using Ampere's law [20],
dt
di E
0
Which state that the rate of change of electric fields produces the current in a conductor.
From the Gauss's law,
E = EdA, E = Eds, or E = EdV
Where dA is a small element of area
ds is a small element of distance
dV is a small element of vollume
From Figure 5.22, E = Eds, is the most suitable express to analyze the voltage
induced in the loop antenna. Hence from Gauss's law again,
Vp = Eds
Showing potential across the point P is an integration of electric fields. From Figure
5.22,
20
Pr
dq
4
1V (From Gauss Law)
220
p
zR
q
4
1V
At the loop center where z = 0,
R4
qV
0
p
So, it is clearly since that the radius of loop plays an important role to determine the
potential difference across the terminal!
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CHAPTER 6: CONCLUSIONS AND RECOMMENDATIONS
6.1 Conclusion
This project has achieved the objectives requirement. As seen in the results, the
antenna can operate at 900MHz or near to 900MHz. The gain is more than 2dBi shown
in the simulation result. At the frequency of 900MHz, the antenna gets resonance and
has lower magnitude of input reflection coefficient, S11. The input impedance of the
antenna also approach 50 and the antenna can receive more than one channel of the
television programme.
The comparison between the simulation results and the practical results on the loop
patch antenna is summarized in table 6.1.
Simulation results Practical resultsS11 = -27.071dB @ 957MHz S11 = -24.622dB@ 840.16392MHz
Zactual = 52.25 + 0.5 @ 957MHz Zactual = 57.440 + j15.552 @ 841.1267MHz
ZL = 45.3 @ 900MHz ZL = 63.346 @ 837.38MHzVSWR = 1.16 @ 900MHz VSWR = 1.385 @ 839.44 MHzGain = 4.8dBi -Directivity = 5dB -
= 85% -
Radiation pattern = Circular -
Table 6.1 - Summarized the comparison results between simulation and practical.
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From the testing of antenna with television channels reception, it is seen that the loop
patch antenna has better performance compared to the commercial type of loop antenna.
6.2 Problem Facings
There are few problems faces while doing the project. These problems are
highlighted as show below:
1. Soldering lead does affect the performance of antenna.
Solution: Tune the antenna by adjust the position so that it resonance at 900MHz.
2. The markers point in the simulation and network analyzer can located at the exact
frequency of 900MHz.
Solution: Use approximation frequency to justify its parameters.
3. The radiation pattern cannot be tested practically.
Solution: Depends on the simulation results.
6.3 Recommendation
In future, the project can be improved to detect the satellite TV signals which operate
at KU band and above. It is also interesting to improve the antenna so that it can receive
the WiFi signal.
Apart from the improvement, an auto searching of the channels also can be added it
into the antenna so that searching of strong signal is done automatically
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REFERENCES
[1] Baker, D.E. (1) and C.A. Van der Neut: “A Compact, Broadband, BalancedTransmission line Patch Antenna from Loops”, IEEE Ant. Prop. Soc. Symp., pp. 568– 570. Albuquerque, 1982.
[2] Kerr, J.L. (1): “Short Loop Axial Length Broad Band Antenna,” IEEE Tans. Ants.Prop., AP-21, 710 – 714, September 1973.
[3] Shin, J.(1) and D.H. Schaubert: “A parametric Study of Loop Patch Antenna,” IEEETrans. Ant. Prop., 47, 879 – 886, May 1999.
[4] Kraus, J.D. (4): “Characteristic of Antennas with Closely-Spaced Elements,” Radio,no.236, 9-19, February 1939.
[5] Kraus, J.D. (6):” W8JK Loop Array Beam Antenna,” QST, 54, 11-14, July 1970.
[6] Bagby, C.K. “A Theoretical Investigation of Electromagnetic Wave propagation onthe Loop Antenna,” Master’s thesis, Electrical Engineering Department,Ohio State University. 1948.
[7] DuHamel, R.H. and A.R. Mahmad: Chap. 28 in R.C. Johnson (ed.), RadioEngineering Handbook, 3rd ed., McGraw-Hill, New York, 1993.
[8] Lindenblad, N.E. “Antennas and Transmission Lines at the Empire State TelevisionStation,” Communications, 21, 10-14, 24-26, April 1941.
[9] Yagi, H. “Loop Patch Antenna Design,” Proc. IRE., 16, 715 – 740, June1998.
[10] RRL(1), Radio Research Laboratory staff, Very High Frequency Techniques,McGraw-Hill, 1974, Chap.4.
[11] Jordan, E.C., G.A. Deschamps, J.D. Dyson and P.E. Mayes, “Developments inBroadband Antennas,” IEEE Spectrum, 1, 58-71, April 1964.
[12] Ballantine, Stuart. “Reciprocity in Loop Patch Antenna”, Proc. IRE, 17, 929 – 951,June 1997.
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LOOP PATCH ANTENNA DESIGNBY ABUBAKAR MAHDI ALHAJI
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[13] Garson, J.R. “Reciprocal Theorems in Antenna Communication,” Proc. IRE, 17,952 – 956, June 1929.
[14] Cox, C.R. “Mutual Impedance between Loop and the Ports,” Proc. IRE, 35, 1367 –1370, November 2000.
[15] Labus, J., “Recherische Ermittlung der Impedanz von Antenna,”Honchfrequenztechink und Electroakustik, 17, January 2001.
[16] Brown, G.H. and O.M. Woodward, “Experimentally Determined ImpedanceCharacteristics of Loop Antennas,” Proc. IRE, 33, 257-262, April 2001.
[17] King, H.E., “Mutual Impedance of Two Loop Antennas in Echelon,” IEEETrans. Ants. Prop., AP-5, 306 – 313, July 2002.
[18] King, Ronold and C.W. Harrison, Jr., “The Distribution of Current along aSymmetrical Loop Antenna,” Proc. IRE, 31, 548 – 567, October 2002.
[19] Lindenblad, N.E.. “Antennas and Transmission Lines at the Empire StateTelevision Station,” Communications, Vol.20, p. 13, May 2003.
[20] E.F. Collin, "Electromagnetic Field Theory", McGraw-Hill Book Co., New York,
2004.
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APPENDIX A: RADIO FREQUENCY SPECTRUM
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APPENDIX B: INPUT IMPEDANCE OF LOOP ANTENNA GRAPHS
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APPENDIX C: LAYOUT OF LOOP PATCH ANTENNA
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APPENDIX D: PRICE LIST
ITEMS PRICE
1. FR4 (20cm x 20cm) RM 12
2. Soldering gun x 1 RM 78
3. Soldering lead x 1 RM 17
4. PCB stand x 4 RM 2.80
5. Transparent plastic board (30cm x 30cm) RM 59
6. Travelling RM 300
7. Iron Chloride RM 46
8. Drill RM 500
9. RF port/SO 239 RM 34
10. TV antenna RM 30
Total RM 1078.80
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APPENDIX E: GANTT CHART