IOSR Journal of Electronics and Communication Engineering (IOSR-JECE)
e-ISSN: 2278-2834,p- ISSN: 2278-8735.Volume 10, Issue 5, Ver. II (Sep - Oct .2015), PP 28-34
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A Review on Recent Ternds and Developments in the Design and
Application of Yagi Uda Antenna
[1]
Hemjith M, [2] Anoop Bk, [3] Manoj Kc
[1]
II Sem MTech C&SP, VJEC, [2] Assistant Prof. ECE, VJEC,[3] Assistant Prof. ECE, VJEC
Abstract: The basic components of any communication system that act as connecting links between the
transmitter and free space or free space and the receiver are called antennas .There are many type of antennas.
Yagi Uda antenna is an important type of antenna.Yagi Uda antenna has many advantages over other
conventional antennas and thus they have a wide range of applications. This paper gives a review about the
recent trends and developments in the area of Yagi Uda antenna design ,simulation and development.
Key terms: Antenna, Yagi Uda antenna, Simulation, Design
I.
Introduction
Antennas are the part of wireless communication systems that converts the electronic signals
(propagating in the RF Trans-receiver) into Electromagnetic Waves (Propagating in the free space) .The
selection, position and design of the antenna suite heavily influences the performance characteristics of the
parent system. Antennas can be classified based on Frequency, aperture, polarization and radiation pattern. The
performance parameters of antennas are Gain, Directivity, Beam area and beam efficiency, radiation pattern,
VSWR/Return loss, polarization and Efficiency. One of the most important type of antenna is the Yagi-Uda
antenna. These antennas are used in fixed-frequency applications as the frequency range over which it has high
gain, is narrow, a few percent of the center frequency, and decreases with increasing gain.
II.
Yagi Uda Antenna
Yagi-Uda antenna is a directional antenna consisting of multiple parallel dipole elements in a line. A
Yagi-Uda antenna consists of a single driven element , a reflector and one or more directors. Reflector element
is slightly longer than the driven dipole, whereas the directors are a little shorter. A substantial increase in the
antenna's directionality and gain can be achieved using this design.Yagi-Uda antenna was invented by Shintaro
Uda and Hidetsugu Yagi in the year 1926and were first widely used during World War II in radar systems. After
that these antennas were used in war they saw extensive development as home television. Yagi-Uda antenna is
also called as "beam antenna",The antenna is used as a high-gain antenna on the HF, VHF and UHF bands. The
Yagi-Uda antenna has a moderate gain which depends on the number of elements. The physical structure of the
Yagi-Uda antenna can be explained below. It consists of a single driven element driven in the center and a
variable number of parasitic elements, a single reflector on one side and optionally one or more directors on the
other side. The parasitic elements serve as resonators, reradiating the radio waves to modify the radiation pattern
and are not electrically connected to the transmitter or receiver. The spacings between elements vary depending
on the design. The directors has a length slightly shorter than that of the driven element .The reflector(s) has a
length longer than that of the driven element. The Yagi Uda antenna has a unidirectional radiation pattern ..The
gain of the antenna can be increased by increasing the number of parasitic elements used. The bandwidth of the
antenna gets narrowed as the number of elements used increases . The size of the reflector will be 5% longer
than the driven element and the directors will be 5% shorter. The length of the Driven Element, the length of
the Directors, the length of the Separation between Directors, the length of the Radii of directors and the length
between driven element and parasitic elements are the important physical parameters to be considered while
designing a Yagi Uda antenna.
III. Working Principle
The driven element of the Yagi Uda antenna is the only member of the structure that is directly excited
and all the other elements are considered parasitic, that reradiate power which they receive from the driven
element The parasitic element is a normal dipole element fed at its centre, with a short circuit across its feed
point. A short circuit reflects all of the incident power 180 degrees out of phase. The operation of the parasitic
element can be modeled as the superposition of a dipole element receiving power and sending it down a
transmission line to a matched load, and a transmitter sending the same amount of power up the transmission
line back toward the antenna element. The superposition of the two voltage waves would give zero if the
transmitted voltage wave were 180 degrees out of phase with the received wave at that point. The reflector
element has an inductive reactance .This means that the phase of its current lags the phase of the open-circuit
DOI: 10.9790/2834-10522834
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A Review on Recent Ternds and Developments in the Design and Application of Yagi Uda Antenna
voltage that would be induced by the received field. The director element has a capacitive reactance with the
voltage phase lagging that of the current. The radio waves radiated by the driven element and those reradiated
by the parasitic elements all should arrive at the front of the antenna in phase, so they superpose and add,
increasing signal strength in the forward direction. In order to achieve this,the elements are given the correct
lengths and spacings.
IV.
Advantages And Application Of Yagi Uda Antenna
Yagi-Uda antennas are directional antennas. They are used for such applications as radio location,data
communications and TV receiving antennas. Yagi-Uda antennas they are usually employed in HF,VHF and
UHF systems . These antennas are also recently used in data transmission in sensor networks and RFID
applications where the radiated power of the source is very limited. Yagi-Uda Antenna is widely used due to its
high gain capability, low cost and ease of construction. These antennas are used in systems where the range of
frequencies in use is fairly small. The Yagi Uda antenna provides long range and high rejection . The tight RF
bandwidth and narrow beam-width is the most highlighting feature of the Yagi Uda antenna.Optimization of the
Yagi-Uda Antenna can be achieved by simulating the radiation patterns for various lengths of the elements and
the spacing between them.
V.
Recent Trends
Due to the large number of advantages and applications of the Yagi Uda antenna many research has
been done on the yagi uda antennae to improve the efficiency and performance .Additional applications of yagi
uda antennae has been developed as a result of advanced research and studies. Many papers has been published
about developments in application and design of yagi Uda antenna. A compact planar directive Yagi-Uda
antenna for A modified two-element Yagi-Uda antenna with tunable beams in the H-plane that includes
forward, backward, omni-directional, and bi-directional beams were designed and simulated. The short-circuit
position of the transmission line connected to the parasitic element is adjusted to obtain the tunable beams. The
current relations between the driven and parasitic elements where studied. The physical dimensions of the
antennae was a important design feature .The length of the driven element was 162.3mm, the length of the
parasitic element was 148.2mm the length of the Separation between the two elements was 77.7mm the length
of the Length of the balun was 87mm, the length of the Radius of the driven element was 1.05mm , the length
of the Radius of the parasitic element was 1.05mm, the length of the Radius of the balun was 1.05 mm, the
length of the Radius of the transmission line was 1.05 mm, the length of the Separation of the balun was
10mm and the length of the Separation of the transmission line was 10mm[2].
A compact linearly polarized high gain antenna for a handheld UHF RFID reader using a Yagi Uda
type antenna with physical dimension of 100 mm x 100 mm was developed. A gain of 6 dB and VSWR better
than 1.3 in approximately 50 MHzband around either European or US RFID bands(865- 870 MHz or 902-928
MHz) was obtained [3]. A high bandwidth Yagi-Uda antenna embedded on a microstrip chip for dedicated
short-range communications was designed and developed.. The Yagi - Uda microstrip antenna developed had a
bandwidth of 33.09% , better gain and front to back ration over a fractional bandwidth superior than 33% with
voltage standing wave ration of more than or equal to 2:1.Due to its small size and improved bandwidth the
developed antenna was recommended for in the field of short – range wireless communication[4]. A 60-GHz
millimeter-wave on-chip Yagi Uda antenna fabricated with a 0.18-μm CMOS process. Coplanar waveguide
(CPW)technology is use to design the feeding network . Thephysical dimension of the antenna was 1.1 × 0.95
mm2. The antenna input VSWR was less than two from 55 to 65 GHz. The measured maximum antenna power
gain is about −10 dBi. The radiation efficiency was about 10%[5]. A novel broadband planar antenna based on
the classic Yagi–Uda dipole array was developed. This antenna achieved 48% bandwidth for VSWR 2, better
than 12 dB front-to-back ratio, smaller than 15 dB cross polarization, 3–5 dB absolute gain and a nominal
efficiency of 93% across the operating bandwidth. Optimization of the antenna is done using finite-difference
time-domain. A gain-enhanced design is presented.Higher gain has been achieved at the cost of reduced
bandwidth. The antennas were realized on a high dielectric constant substrate . These antennas are completely
compatible with microstrip circuitry and also with solid-state devices[6] .The overall dimension of a microstrip
antenna was reduced using a partially filled high-permittivity substrate. A microstrip Yagi Uda antenna with
reduced size for a repeater system in a mobile communication cellular band (824–894 MHz)was designed .The
antenna manufactured accourding to thus design was lightweight and smaller in size[7] .
A Microstrip Yagi-Uda antenna, operating very near to resonant frequency 900MHz with relative
permittivity 2.2 for RT Duroid 5880 substrate, height of substrate 1.575 mm, characteristicimpedance 50 ohm
and thickness of strip conductor 35μm was developed. To have low profile, Yagi Uda antennas are implemented
using microstrip circuits. The gain of an antenna array with a very simple feeding can be enhanced by using this
type of structure. The antenna consisted of patch as a driven element, and printed dipole for parasiticelements .
The design enable the manufacturing of the antenna at low cost. A gain of 8.33 dB is obtained.
DOI: 10.9790/2834-10522834
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A Review on Recent Ternds and Developments in the Design and Application of Yagi Uda Antenna
Increaseddirectivity in the direction of satellites can be obtained for ground station application. The performance
can be further improved byapplying defective ground structure or frequency selective surface. Minimization can
be obtained by optimizing dipoles width[8]. An Ultra Wide Band Microstrip Yagi Uda antenna was developed
with very good performance at theoperating frequencies 0.85, 2.4, 3.5 and 5.2 GHz. A 20 to -40 dB return loss
at the bands 0.85, 2.4, 3.5, 4.5 and 5.2 GHz and VSWR less than 1.7 at these frequencies were obtained from the
simulation results. Finite element method (FEM) of simulation was applied by using HFSS simulator to obtain
the optimized parameters so that the best design for the antenna can be obtained [9].
A planarsix element microstrip Yagi-Uda antenna is successfully simulated and developed. The
microstrip Yagi-Uda antenna developed was a highly directional antenna operating at a frequency of 6.52 GHz.
CST simulation software was used to simulate the antenna. The substrate used for fabricating the antenna was
FR4 having a dielectric constant of 4.3, supported substrate thickness of 1.6mm and loss tangent of 0.02. The
antenna has a wideband and directional radiation pattern with very high gain and effective radiation efficiency.
The antenna can be effortlessly used it C-Band of Microwave frequency. Depending up on the applications gain
of this antenna can be varied by varying dimensions of its ground-plane[10]. A dual-frequency
circularlypolarized electronically steerable microstrip patch antenna array was developed which is suitable for
land-mobile communications. The four antennas forming the array are located radially from a single square
reflector patch on a double-sided printed circuit board based on a four element Yagi-Uda patch antenna,. The
main lobe of the array covers the elevation angles from 20 to 70. A peak gain of 8.4 dB is obtained at a
frequency of at 1.54 GHz and a peak gain of 11.7 dB is obtained at a frequency of 1.62 GHz. By electronically
switching between the four elements, a full azimuthal coverage is made possible [11].
A compact 3D U-shaped Yagi-Uda antenna with different high permittivity and permeability materials
was developed and studied. Antennas made of material with high permittivity and permeability dielectrics which
allow the enhancement of light and high frequency RF communication and sensing are required for high speed
data processing at nanometer wavelength. The main important feature of the Optical Yagi- Uda antenna is its
unique directive property which mobilizes the concepts of beam forming and beam scattering .ANSYS HFSS
v15.0 simulation software is the software that is used for the simulation of this antenna with the changes in
dielectric permittivity and permeability and the spacing between the elements is relying on the operating
wavelength [12]. A printed Yagi-Uda antenna with an integrated balun for WLAN applications was designed
and simulated. The operating frequencies of the planar directive antenna is designed at 2.4 GHz and 5 GHz
frequency bands. The feed to the antenna is an integrated balun in the form of microstrip-to-coplanar strips
(CPS) transition. FR4 with a dielectric constant of 4.4 and thickness 1.6mm is used as the substrate[13]. A high
gain broadband Yagi-Uda antenna for wireless communication application at frequency of 5.2 GHz was
developed. The simulation software used for the design of the antenna was HFSS simulation software. FR-4
with dielectric constant of 4.4 and height of 1.6 mm is used as the substrate used to design the antenna. A high
gain with wide bandwidth can be obtained by using this antenna[14].
A microelectromechanical system (MEMS) reconfigurable Yagi Uda antenna with a new architecture was
designed and simulated. The antenna designed is a reconfigurable Yagi-Uda antenna with one dipole, one
reflector and three directors.The antenna is designed in a micro scale such that it changes the length of those
elements according to the desired frequency in the range from75 to 100GHZ. [15]A microstrip Yagi-Uda array
design has been simulated at frequency of 6.95 GHz. The software used for simulation of Yagi Uda array is the
CST MW Studio Software. The reflector, directorand driven element are designed by using microstrip patches
of different dimensions. The substrate is FR-4 lossy at height1.6mm and loss tangent of 0.02. Very high gain
and effective radiation efficiency can be achieved by this design. The antenna has a very less return and very
good compatibility with microwave circuitry[16]. A Yagi-Uda Ultra Wide Band Micro strip antenna operating
frequencies 7 GHz was developoed. The designed antenna has a antenna good front to back ratio and good
return loss of 7 GHz and VSWR less than 1.7 at these frequencies. The antenna has two sections of reflector
element and one driven element and one director. Micro strip line is used to feed the antenna. ANSOFT HFSS13 design software is used[17].
DOI: 10.9790/2834-10522834
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A Review on Recent Ternds and Developments in the Design and Application of Yagi Uda Antenna
VI.
ANTENNA
SUBST
RATE
Compact
Planar
Directive
Yagi Antenna
For Wlan
Application
FR4 of
dielectri
c
constant
4.4
Modified
Two-Element
Yagi-Uda
Antenna
With Tunable
Beams
Compact
Yagi Antenna
for Handheld
UHF RFID
Reader
Comparison Table
PHYSICAL
DIMENSIO
N(mm)
24 mm x 30
mm
GAI
N
(db )
5
OPERATING
FREQUENC
Y
5 GHz
APPLICATI
ON
-
L1 -162.3
L2-148.2
Sp- 77.7
Sb -87
a -1.05
b -1.05
c-1.05
d- 1.05
Wb-10
Wd-10
St- 74
-
850MHz
modern
wireless
communicatio
n
systems
ABS
plastic
(dielectr
ic
permitti
vity 3.5)
100 mm
x 100 mm
6
US and
European
(ETSI) UHF
RFID bands
(902928 MHz and
865-870 MHz)
UHF-RFID
Reader
-
-
10
High
Bandwidth
Yagi-Uda
Antenna For
Dedicated
Short Range
Communicati
ons
A 60-Ghz
MillimeterWave CPWFed Yagi
Antenna
Fabricated By
Using 0.18Μm CMOS
Technology
high frequency
(HF) and
Ultra-high
frequency
(UHF) bands,
usually
between 3
MHz to 3
GHz.
-
The CMOS
antenna chip
size is
1.1mm ×
0.95 mm
DOI: 10.9790/2834-10522834
10
60GHZ
WLAN
DESIG
N
TOOL
CADFE
KO
softwar
e.
NEC
softwar
e,
method
of
moment
s-based
numeric
al
electro
magneti
c code
(NEC)
HFSS
Short range
communicatio
n
High
Frequen
cy
Structur
e
Simulat
or
(HFSS)
softwar
e
WPAN
The
HFSS
FEMbased
3-D
fullwave
electro
magneti
c solver
is used
for the
design
simulati
on.
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JOURNA
L
Internation
al Journal
of
Electrical,
Electronic
s and Data
Communi
cation
Progress
In
Electroma
gnetis
Research
Intermec
Technolog
ies,
Everett,
WA
98203
Internation
al Journal
of
Computer
and
Communi
cation
System
Engineerin
g
IEEE
electron
device
letters
31 | Page
A Review on Recent Ternds and Developments in the Design and Application of Yagi Uda Antenna
A BroadBand Planar
Quasi-Yagi
Antenna
Duroid
with
dielectri
c
constant
10.3
Design And
Development
Of Microstrip
Yagi-Uda
Array For
900mhz
Frequency
RT
Duroid
5880
substrat
e
A Novel Ultra
Wide Band
Yagi
Microstrip
Antenna For
Wireless
Applications
-
Highly
Directional CBand Planar
Six Element
Microstrip
Yagi-Uda
Antenna
(FR-4,
lossy)
with
dielectri
c
constant
of 4.3,
Yagi Uda
Antenna With
Integrated
Balun For
WLAN
Application
FR4 of
dielectri
c
constant
4.4
Design Of 5.2
Ghz YagiUda Antenna
FR-4
with
dielectri
W1 = W3 =
W4 = W5 =
Wdri = Wdir
= 0:6, W2 =
1:2,
W6 = S5 =
S6 = 0:3, L1
= 3:3, L2 =
L5 = 1:5, L3
= 4:8,
L4 = 1:8,
Sref = 3:9,
Sdir = 3:0,
Ssub = 1:5,
Ldri = 8:7,
and
Ldir = 3:3.
L=
110.8mm,
W=131.8m
m
3-5
9.5GHz
High Gain
Applications
-
IEEE
Transactio
ns On
Antennas
And
Propagatio
n
8.33
900MHz
Industrial and
Medical
Application
Ansoft
HFSS
-
-
(0.85, 2.4, 3.5,
4.5 and 5.2)
GHz
Ultra Wide
Band
Applications
HFSS
L=5.8,L1=2.
5
W=1.0,
W1=0.6,
S1= 0.87,
S2=2.8,
S3=3.4,
S4=2.4,
L1=3,V=2,
X=2.5,
Y=3,Z=3.5
24mm x
24mm
-
6.25GHz
C-Band
Applications
HFSS
IEEE
Sponsored
Internation
al
Conferenc
e on
Innovation
s in
informatio
n,Embedd
ed and
CommnS/ms
Journal of
Theoretica
l and
Applied
Informatio
n
Technolog
y
Internation
al Journal
of
Emerging
Technolog
y&
Research
4–
4.5
2.4 GHz and 5
GHz
WLAN
-
7
5.2GHz
WLAN,
NGMN and
other wireless
DOI: 10.9790/2834-10522834
CADFE
KO
softwar
e.
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HFSS
Internation
al Journal
of
Computer
Applicatio
ns
Internation
al Journal
of
32 | Page
A Review on Recent Ternds and Developments in the Design and Application of Yagi Uda Antenna
For Wireless
Communicati
on
Application
c
constant
of 4.4
communicatio
n applications
Microstrip
Patch YagiUda Array
For
Millimeter
Wave
Applications
FR4
L=85,W=40,
L1=9.5,W1=
14,L2=12.6,
W2=17,L3=
15.6,W3=20
.45,L4=,W4
=31.8.
4.76
6.95GHz
Industrial and
medical
Applications
A New YagiUda
Microstrip
Antenna With
Good F/B
Ratio
RT
Duroid
5880
which
has
relative
permitti
vity
2.23.
L= 14.038
mm
PD=10.74m
m
PR=11.277
mm
PR1=5.6385
mmPR1=5.6
385mm
PP=10.203m
m
W=
16.595mm
-
7GHz
Ultra Wide
Band
Application
CST
simulati
on
softwar
e.
ANSOF
T
HFSS13
Advanced
Research
in
Electronic
s and
Communi
cation
Engineerin
g
Internation
al Journal
of
Engineerin
g
Research
and
General
Science
Internation
al Journal
of
Scientific
&
Engineerin
g
Research
VII. Conclusion
Yagi uda antenna is a very important type of antenna that finds application in different areas of wireless
communication.Due to this immense advantages and applications, many research and studies has been
conducted on this antennae.Design of yagi Uda antenna for applications other than the conventional ones are
discussed in many papers.This paper put forward a summary of recent developments and studies that has been
occurring in the application and design of Yagi Uda antennae
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DOI: 10.9790/2834-10522834
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