International Journal of Application or Innovation in Engineering & Management... Web Site: www.ijaiem.org Email: , Volume 2, Issue 6, June 2013

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International Journal of Application or Innovation in Engineering & Management (IJAIEM)
Web Site: www.ijaiem.org Email: editor@ijaiem.org, editorijaiem@gmail.com
Volume 2, Issue 6, June 2013
ISSN 2319 - 4847
Finite Element Modelling and Analysisof
Archimedean Spiral Slot Antenna
1
Sunisha Rani,2Anupma Marwaha
1
M.Tech Research Scholar, ECE Department ,SLIET Longowal, Punjab -148106 India
2
Associate Professor,ECE Department, SLIET Longowal, Punjab -148106 India
Abstract
Spiral slot antenna is widely used due to its low profile, light weight, high efficiency, circular polarization, broad bandwidth
and conformal design.An analysis of resonant behaviour ofArchimedean spiral slot antenna with different number of turnsis
presented in this paper operating in frequency range between 1 GHz to 5 GHz. The Archimedean spiral slot antenna is
patterned on a thin single sided metal substrate. The lumped port is placed at the centre of the spiral slot to excite the antenna,
Rogers RO4003 substrate is used with dielectric constant of 3.38. FEM based COMSOL Multiphysics software is utilised for the
spiral antenna simulation and modelling. It has been observed that with increase in number of turns of the spiral slot antenna,
the bandwidth of antenna increasesas well as there is increase in the directivity of the antenna. There is further shift of
resonant frequency towards lower side with increase in number of turns. The proposed Archimedean spiral slot structuremay
be used ashighly directive antenna for S-band applications.
Keywords: Archimedean Spiral slot antenna, S- Band, Microstrip antenna, FEM
1. INTRODUCTION
The rapid development in personal and computer communication technologies demands the combination of more than
one communication systems into a single compact element. This implies that the future communication terminal
antennas must meet the necessities of multi-band or wideband to sufficiently cover the possible operating bands
[1].Spiral slot antennas are gaining importance due to their extensive bandwidth, high efficiency, low profile and stable
impedance characteristic over the last two decades[2].Microstrip antennas are one of the most broadly used types of
antennas in the microwave frequency range both as single elements and (more often) in array configurations. Their
advantages are well known i.e. itslow cost, conformity, ease of fabrication and integration, reproducibility, ruggedness,
light weight, and low profile.Narrow bandwidth and poor efficiency are top subjects that affectthe microstrip antenna
performance [3].There are many methods to increase the performance limitations of microstripantenna. One of the
method which is widely used and drawing the interest of researchers is slotting [4].Slotting is done to increase the
bandwidth and also for notching the unwanted frequency band with theinsertion of various shaped slots like narrow
shaped slots, wide slots, circular ring slot, U shaped slots on antenna patch or substrate. Because of extremely thin
profile (0.01 to 0.05 wavelength),microstrip slot antennas have createextensive applications in military aircraft,
missiles, rockets and satellites [5-6] with operating frequencies in S-bandranging from 2 to 4 GHz.The S band
frequencies are used inweather radar, surface ship radar and some communication satellitesespecially those used by
NASA to connect with the Space Shuttle and the International Space StationSystems. In this paper anArchimedean
spiral slot antenna has been designed to analyse the relationship between the resonant performances of the antenna with
the change in the number of the turns. The radiation properties have also been observedand it has been observed that
they are nearly similar in nature.
2.ARCHIMEDEAN SPIRAL SLOT ANTENNA
Archimedean spiral slot antenna is essentially afrequency independent microstrip patch antenna,however the design
parameters of the antenna can be optimized to achieve the desired bandwidth, gain and radiationpatterns [7].It radiates
from a region where the circumference of the spiral equals one wavelength, called the active region of the spiral. Each
arm of the spiral is fed 180° out of phase, so when the circumference of the spiral is one wavelength the current at
opposite points on each arm of the spiral add in phase in the far field. The low frequency operating point of the spiral is
determined theoretically by the outer radius and is given by [8]
= (c/2 )
(1)
Wherec is the speed of light.Likewise the high frequency operating point is determined by the inner radius,
= (c/2 )
(2)
In practice the low frequency point will be greater than the predicted value of Eqn. (1) due to reflections from the end
of the spiral. The reflections can be minimized by using resistive loading at the end of both arm or by adding
conductivity loss to specific part of the outer turn of botharm.
Volume 2, Issue 6, June 2013
Page 185
International Journal of Application or Innovation in Engineering & Management (IJAIEM)
Web Site: www.ijaiem.org Email: editor@ijaiem.org, editorijaiem@gmail.com
Volume 2, Issue 6, June 2013
ISSN 2319 - 4847
Figure.1Geometry of Archimedean spiral slot antenna
As shown inFigure. 1, an arm of an Archimedean spiral is linearly proportionate to the angle, φ, and is defined by the
following relationship
r = aφ+ r_0(3)
Eqn. (3) states that the radius r of the antenna increases linearly with the angle φ, where r_o is inner radius of the
spiral, a is the constant which controls the growth rate, andφ is the azimuthal angle progression.
3. FEMMODELING OF ARCHIMEDEANSPIRAL SLOT ANTENNA
The RF module of COMSOL Multiphysics is used to carry out the simulations. TheArchimedean spiral slot antenna is
constructedwith two armspatterned on a thin single sided metal substrate using parametric curves. The metal surface is
modelled as perfect electric conductor assuming the conductivity is very high and loss on the surface is ignorable.
There are many ways to feed the antenna. Here a lumped port is chosen in order to feed the antenna and it islocated at
the centre of the spiral slot to excite the antenna. The antenna structure and air region are enclosed by a perfect
Matched layer (PML). In this paper value of r_ois taken as 1.5mm, while the values of φ are taken as 5π, 6π and 7π for
2.5, 3 and 3.5 turns respectively. The antenna is generated using Rogers RO4003substrate material with dielectric
constant of 3.38.
4.RESULTS AND DISCUSSION
The simulation tool adopted for evaluating the performance of the proposed antenna is COMSOL software, which
exploits the FEM to solve the electric field integral equation. Table.1 shows the resonant performance characteristics of
the Archimedean spiral slot antenna with different number of turns. The analysis is performed considering three cases
of variation in number of turns i.e.2.5, 3 and 3.5 respectively. It is observed that with increase in the number of turns
the bandwidth increases. Furtherit is illustrated that resonant frequency shift towards lower side with increase in the
number of turns of spiral slot antenna.
Table.1 Comparison of resonant performance characteristics
No. of
turns
Resonant Return
Frequency loss
(GHz)
(S11)
Bandwidth Beamwidth
(h)
(degrees)
2.5
4.5
-15.1
68.8%
65
3
3.5
-12.8
88.5%
68
3.5
3
-12.3
120%
62
The resonating characteristics are also illustrated in Figure.2 by plotting the S-parameter, S11for the antenna and from
the figure it is clear that the antenna the value S11 remains below 10dB at all the frequencies greater than 2.392GHzfor
2.5 turns of spiral and further beyond 1.912GHz and 1.462 GHzfor the number of turns as3 and 3.5 respectively thus
justifying the very wideband response with maximum number of turns.With these resonant properties the proposed
antenna is feasible for S-band applications.
0
2.5 turn
3 turn
3.5turn
-2
-4
dB
-6
-8
-10
-12
-14
-16
1
1.5
2
2.5
3
3.5
frequency in GHz
4
4.5
5
Figure. 2 Return loss S11 for varying spiral turns
Volume 2, Issue 6, June 2013
Page 186
International Journal of Application or Innovation in Engineering & Management (IJAIEM)
Web Site: www.ijaiem.org Email: editor@ijaiem.org, editorijaiem@gmail.com
Volume 2, Issue 6, June 2013
ISSN 2319 - 4847
The radiation characteristics of the Archimedean spiral slotantenna for different turns are shown from Figure. 3 to
Figure. 5 and it has been observed that they are nearly similar in nature. The radiation pattern is bidirectional radiation
pattern on yz-plane. The frequency independent behaviour is also evident from the characteristics.Maximum directive
with 62obeam width is achieved in the case of 3.5 number of turns of the spiral slot antenna.
Figure.3 Radiation pattern at resonating frequency 4.5 GHz on yz –plane
Figure.4 Radiation Pattern at resonating frequency 3.5 GHz on yz - plane
Figure.5 Radiation Pattern at resonating frequency 3 GHz on yz- plane
5. CONCLUSIONS
The FEM based COMSOL simulation softwareis used here for the design, modelling and analysis of Archimedean
spiral slot antenna. The resonant performance of the antenna with different number of turns of the spiral has been
considered to illustrate the frequency independent behaviour.It has been demonstrated that by keeping the antenna
parameters as constant and with increase in onlynumber of turns of antenna bandwidth of the antenna increases and
best directivity is obtained at spiral having 3.5 turns. Also the resonant frequency of the antenna shift towards the lower
frequency side with the increase in number of turns of the spiral slot antenna. The spiral slot antenna is feasible for use
for S-band applications.
References
[1.] Wang, F. J. and J. S. Zhang, “Wide band cavity-backed patch antenna for PCS/IMI2000/2.4 GHz WLAN,”
Progress InElectromagnetics Research, PIER 74, 39–46, 2007
[2.] Kaiser, J. A., “The Archimedean two-wire spiral antenna," IRE Trans. Antennas and Propagation, Vol. 8, No. 3,
312-323, 1986.
[3.] Ramesh Garg, ParkashBhartia, Inderbahl, ApisakIttipiboon , “ Microstrip Antenna Design Handbook ’’, A .V.
Title. VI series.
[4.] K. Siakavara , “ Methods to Design Microstrip Antennas for Modern Applications ” , Aristotle University of
Thessaloniki, Dept. of Physics, Radiocommunications Laboratory, Thessalonik, Greece.
[5.] F.Yong, X. Zhang, X. Ye, and Y. Rahmat-Samii, “Wide-band E-shaped patch antennas for wireless
communication," IEEE Trans.on Antennas Propagat., Vol. 49, No. 7, pp.1094-1100, Jul. 2001.
[6.] Jen-Yea Jan and Jia-Wei Su, “Bandwidth enhancementof a printed wide slot antenna with a rotated slot,” IEEE
Transaction and Antennas Propagation., Vol.53, No.6, pp.2111-2114, June 2005
[7.] ConstantineA. Balanis, “Antenna Theory analysis and design’’, 2nd edition, John Wiley and sons.
[8.] http:/scholar.lib.vt.edu/theses/available/etd-01082002073223/unrestricted/caswell_etd_ch2.pdf
Volume 2, Issue 6, June 2013
Page 187
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