2 Atinder Pal Singh 643 Research Article Apr 2012
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Transcript of 2 Atinder Pal Singh 643 Research Article Apr 2012
Available ONLINE www.vsrdjournals.com
VSRD-IJEECE, Vol. 2 (4), 2012, 160-167
____________________________
1,3Research Scholar, 2Assistant Professor, 1,2,3Department of Electronics Technology, Guru Nanak Dev University, Amritsar, Punjab, INDIA. *Correspondence : [email protected]
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Design of Edge Fed Rectangular Microstrip Patch Antenna for WLAN Applications
Using Ansoft-HFSS 1Atinder Pal Singh*, 2Ravinder Kumar and 3Hartej Singh Dadhwal
ABSTRACT
As of today, Wi-Fi (also known as WLAN) has become a standard in most computers. Almost every modern
mobile phone and other gadgets are being implemented with Wi-Fi technology. Wi-Fi makes it possible for the
user to connect to the internet or LAN (Local Area Network) though a wireless connection hence its other name
is WLAN. WLAN uses the technical term “IEEE 802.11” and has standards in the names of 802.11 b/g/n.
Microstrip Patch Antennas have been widely used in a various useful applications, due to their low weight and
low profile, conformability, easy and cheap realization. In this paper, an attempt has been made to design Edge
Fed Microstrip antenna structure for WLAN systems at 2.4835 GHz Frequency Using Ansoft-HFSS v13.
Keywords : Edge Fed Rectangular Patch Antenna, WLAN, Rogers RT/Duriod 5870 Substrate, HFSS v13.
1. INTRODUCTION
An antenna is a device used to transform an RF signal, travelling on a conductor, into an electromagnetic wave
in free space. Antennas demonstrate a property known as reciprocity, it means that an antenna will maintain the
same characteristics regardless if it is transmitting or
receiving. Most of the antennas are resonant devices, which
operate efficiently over a relatively narrow frequency band.
A Microstrip antenna consists of a metallic pattern on one
side of a dielectric substrate and ground plane on the other
side of the substrate. The antenna patch can have different
shapes, but is most likely rectangular.aaaaaaaaaaaaaaa
Fig. 1 : Structure of Rectangular Microstrip Patch Antenna
Atinder Pal Singh et al / VSRD International Journal of Electrical, Electronics & Comm. Engg. Vol. 2 (4), 2012
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2. VARIOUS SUBSTRATE MATERIALS
2.1. Ceramic Substrate
The ceramic substrate is mainly used in small size applications with frequencies below 1 GHz. It has low a loss
tangent and has good chemical resistance, but is also very expensive. Besides that, ceramic is very hard to
produce and handle. For instance it is very hard to drill holes in the substrate without breaking it. Some ceramic
material has a high dielectric constant which is used where you need an important size reduction.
2.2. Synthetic Substrate
Synthetic substrate is commonly made out of organic material like PTFE (also known as Teflon). These
materials possess low loss tangent and low Er. The only problem is that this material is very soft and can
therefore easily change the characteristics of a microstrip antenna if it is not handled well enough.
2.3. Composite Material Substrate
Composite material is made out of mixed chemicals between fibreglass, ceramic or quartz and synthetic
material. There is a wide variety of composite material on the market which has been modified so they fit both
to antenna fabrication and standard PCB design.
2.4. Low-Cost Low-Loss Substrate
Ceramic, Synthetic and Composite material substrate is usually used where other applications are needed or a
microstrip antenna needs perfection and also it is too expensive to use in consumer electronics such as TV’s,
mobile phones, etc.
3. RESEARCH METHODOLOGY
In order to make performance predictions the rectangular patch antenna has the following parameters, where λ0
is the wavelength in vacuum also called the free-space wavelength.
• Length (L) : 0.3333λ0 < L < 0.5λ0
• Height (h) : 0.003λ0 ≤ h ≤ 0.05λ0
• Thickness (t ) : t << λ0
• Dielectric constant (εr ) : 2.2 ≤ ε r ≤ 12
HFSS (High Frequency Structure Simulator) software is the industry-standard simulation tool for 3-D full-wave
electromagnetic field simulation and is essential for the design of high-frequency and high-speed component
design. This software automatically divides the geometric model into a large number of tetrahedron, where a
single tetrahedron is a four-sided pyramid. This collection of tetrahedron is referred to as the finite element
mesh. Each element can contain a different material. Therefore, the interface between two different materials
must coincide with element boundaries. The value of a vector field quantity (such as the H-field or E-field) at
points inside each tetrahedron is interpolated from the vertices of the tetrahedron. By representing field
Atinder Pal Singh et al / VSRD International Journal of Electrical, Electronics & Comm. Engg. Vol. 2 (4), 2012
Page 162 of 167
quantities in this way, the system can transform Maxwell's equations into matrix equations that are solved using
traditional numerical methods. With HFSS, engineers can extract scattering matrix parameters (S, Y, Z
parameters); visualize 3-D electromagnetic fields (near- and far-field). Each HFSS solver is based on a
powerful, automated solution process where you are only required to specify geometry, material properties and
the desired output. From there HFSS will automatically generate an appropriate, efficient and accurate mesh for
solving the problem using the selected solution technology. The Comparison among various antenna software
packages and their principle of operation are given in the form of table at the end.
4. DATA ANALYSIS
The rectangular patch antenna is approximately one-half wavelength long section of rectangular microstrip
transmission line. When air is the antenna substrate, the length of the rectangular microstrip antenna is
approximately one-half of a free-space wavelength. As the antenna is loaded with a dielectric as its substrate, the
length of the antenna decreases as the relative dielectric constant of the substrate increases. The resonant length
of the antenna is slightly shorter because of the extended electric "fringing fields" which increase the electrical
length of the antenna slightly. In our paper we taken the Substrate material as Rogers RT/Duriod 5870(tm) with
relative permittivity = 2.33, Dielectric Loss Tangent = 0.0012 and Lande G factor = 2. Its low dielectric
constant, low loss tangent and low cost make it a first choice material for microwave substrate. The figure below
shows the various terminologies associated with Edge Fed Microstrip Patch Antenna.
Fig. 2 : Terminology of Edge Fed Microstrip Patch Antenna
There are various theories that can be used in analysis and design of rectangular microstrip patch antennas like
Cavity model, Transmission Line model etc. We have used Transmission Line model here. According to this
model, rectangular patch is viewed as very wide transmission line that is transversely resonating, with the
electric field is varying sinusoidal under the patch along its resonant length. Various Formulae for calculating
the Dimension parameters of Rectangular Microstrip Patch antenna using this model are:
Effective Dielectric Constant :
Atinder Pal Singh et al / VSRD International Journal of Electrical, Electronics & Comm. Engg. Vol. 2 (4), 2012
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Width of the patch:
Due to Fringing fields, the change in dimensions of length is given by:
Effective Length of the patch:
The various design parameters of Edge fed Rectangular patch Antenna are calculated at frequency 2.4835 GHz.
The various parameters are: Patch dimension along x = 4.77cm, Patch dimension along y = 3.99cm, Substrate
Dimension along x = 8.1cm, Substrate dimension along y = 16.67cm, Edge feed width = 0.189cm, Edge feed
length = 2.263cm, Feed Width = 0.485cm, Feed Length = 3.679cm. These parameters are used by the Ansoft-
HFSS to generate the corresponding design of Edge fed rectangular Microstrip patch antenna which is shown in
fig.3.
Fig. 3 : Ansoft-HFSS Generated Edge Fed Patch Antenna
5. EXPERIMENTAL RESULTS
The various Antenna Parameters are calculated by using Ansoft-HFSS and the simulated results are shown
below:
Atinder Pal Singh et al / VSRD International Journal of Electrical, Electronics & Comm. Engg. Vol. 2 (4), 2012
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5.1. Return Loss
Fig. 4 : Return Loss v/s Frequency Curve
5.2. Far Field Radiation Patterns
Fig. 5(a) : Radiation Pattern showing Total Gain
Fig. 5(b) : Radiation Pattern Showing Total Gain at Phi = 0 & 90 degree
Atinder Pal Singh et al / VSRD International Journal of Electrical, Electronics & Comm. Engg. Vol. 2 (4), 2012
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5.3. 2-D Radiation Pattern
Fig. 6(a) : 2-D Total Gain Plot
Fig. 6(b) : 2-D Gain at Phi = 0 & 90 degree
5.4. 3-D Polar Plot
Fig. 7 : 3-D Polar Plot showing Total Gain (in db)
Atinder Pal Singh et al / VSRD International Journal of Electrical, Electronics & Comm. Engg. Vol. 2 (4), 2012
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5.5. Field Distributions
Fig. 8(a) : E-Field Distribution
Fig. 8(b) : H-Field Distribution
Fig. 8(c) : Mesh Pattern of Edge Fed Patch Antenna
Mesh Generation is the practice of generating a polygonal or polyhedral mesh that approximates a geometric
domain to the highest possible degree of accuracy. The triangles show the current distribution. Here the number
of triangles on the substrate is more than on patch thus indicating the current distribution in the substrate is more
than patch.
Atinder Pal Singh et al / VSRD International Journal of Electrical, Electronics & Comm. Engg. Vol. 2 (4), 2012
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6. CONCLUSION
In this Paper, we have investigated the dimensions of Linearly Polarized Edge Fed Rectangular patch antenna on
Rogers RT/Duroid 5870(tm) substrate for WLAN/Wi-Fi applications at a frequency of 2.4835 GHz. The various
performance properties are analyzed for the optimized design using Ansoft-HFSS. Also the Comparison has
been made among various Simulating softwares and their principle of operation in the table shown below.
7. FUTURE SCOPE
In Future, we can compare the results and performance by using Liquid Crystal Polymer, Ceramic substrate or
FR4 instead of Roger RT/Duroid 5870. Apart from that, we can use different feeding methods such as
Microstrip line feed, Probe feed techniques or Elliptical shaped patch can be used instead of Rectangular patch.
Table 1 : Principle of Operation of Various Software Packages used for Microstrip Patch Antennas
Software Name Principle of Operation FEKO Method of Moment HFSS Finite Element Method ADS Momentum Finite Difference Time Domain (FDTD) IE3D Method of Moment CST Microwave Studio Finite Integration Technique
8. REFERENCES [1] A. Vasylchenkot, Y. Schols, W. De Raedtt, G. A. E. Vandenbosch “A Benchmarking of Six Software
Packages for Full Wave Analysis of Microstrip Antennas”.
[2] C.A. Balanis, “Advanced Engineering Electro-magnetics”, John Wiley & sons, New York, 1989.
[3] Gagandeep Sharma, Deepak Sharma, Abhishek Katariya “An Approach to Design and Optimization of
WLAN Patch Antennas for Wi-Fi Applications”, IJECCT 2012,Vol.2(2).
[4] C.A. Balanis, “Antenna Theory”, 2nd Ed., John Wiley & sons, inc., New York.
[5] Atinder Pal Singh, “Various Methods and Software packages for Simulating Microstrip Patch Antennas”,
2nd National Conference on Emerging Trends in Engineering-April, 2012, Page =125-128.
[6] EMSS - EM Software & Systems Ltd, FEKO Suite 5.2 user manual, january 2006.
[7] James, J. R., P. S. Hall, “Handbook of Microstrip Antennas”, Peter Peregrinus, London, UK, 1989
[8] Pozar D. M., “Microstrip antennas," Proc. IEEE, Vol.80, No. 1, 79, 91, Jan. 1992
[9] Zeland Software, Inc., IE3D v. 11.2 user manual, january 2006, http:www.zeland.com.
[10] Narendra Neupane, Shankar Acharya, N.Anil Babu, B.T.P.Madhav, “Linearly Polarized Microstrip
Reatangular Patch Antenna On FR4 Substrate for High Speed WLAN Systems” GJCAT, Vol.1(2),2011.