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IJECT Vo l . 4, Is s u e Sp l - 4, Ap r i l - Ju n e 2013<br />

ISSN : 2230-7109 (Online) | ISSN : 2230-9543 (Print)<br />

<strong>Circularly</strong> <strong>Polarized</strong> <strong>Microstrip</strong> <strong>Patch</strong> <strong>Antenna</strong><br />

<strong>with</strong> T-<strong>Shaped</strong> Slot<br />

1 Sanyog Rawat, 2 K K Sharma<br />

1<br />

Amity School of Engineering and Technology, Amity University Rajasthan, India<br />

2<br />

Malaviya National Institute of Technology, Jaipur, Rajasthan, India<br />

Abstract<br />

In this paper a new geometry of circularly polarized patch antenna<br />

is proposed <strong>with</strong> improved bandwidth. The radiation performance<br />

of proposed patch antenna is investigated using IE3D simulation<br />

software and its performance is compared <strong>with</strong> that of conventional<br />

circular patch antenna. The simulated return loss, axial ratio and<br />

impedance <strong>with</strong> frequency for the proposed antenna are reported<br />

in this paper. It is shown that by selecting suitable slot dimension,<br />

air gap and location of the slots, the impedance bandwidth can<br />

be enhanced upto 10.74% as compared to conventional circular<br />

patch (3.41%) <strong>with</strong> an axial ratio bandwidth of 2.46%.<br />

mm is also added between patch and ground plane, as shown<br />

in fig. 2(a) and (b). Here conventional circular patch antenna<br />

is considered the reference antenna to compare the results of<br />

proposed geometry.<br />

Keywords<br />

<strong>Microstrip</strong> <strong>Patch</strong>, Circular Polarization, Bandwidth, Axial-Ratio,<br />

Circular <strong>Patch</strong><br />

I. Introduction<br />

The antenna manufacturing industry has experienced a significant<br />

growth in the past several years. There is an essential need for a light<br />

weight and good performance antenna for modern communication<br />

applications. In order to meet these demands, microstrip patch<br />

antenna is one of the potential candidate for it. They are suitable<br />

for many applications like mobiles, aircraft, satellite, missile etc.<br />

They are low profile structure, robust in nature, inexpensive to<br />

manufacture, compatible <strong>with</strong> MMIC designs and relatively light<br />

and compact [1]. A microstrip antenna consists of conducting<br />

patch on a ground plane separated by dielectric substrate. The<br />

conducting patch can take any shape like rectangular, elliptical,<br />

square, circular, triangle etc. but rectangular and circular<br />

configurations are the most commonly used geometries [2].<br />

Other configurations are complex to analyze and require heavy<br />

numerical computations. Among the conventional microstrip<br />

antenna geometries, circular microstrip antenna is widely analyzed<br />

antenna due to easy modelling and applicable boundary conditions<br />

[3]. The major drawback of circular microstrip patch antenna is<br />

narrow bandwidth and low gain especially at lower microwave<br />

frequencies [4]. With the insertion of slots in the patch-geometry,<br />

the path of the patch current increases which in turn increases the<br />

impedance bandwidth of an antenna. The skimmer shaped circular<br />

microstrip patch antenna to increase bandwidth up to 4.13% have<br />

been investigated [5] and bandwidth improvement by 2.3 times of<br />

the conventional antenna bandwidth (1.4%) using slots in circular<br />

microstrip patch antenna is also investigated in past [6].<br />

There is another easy way to improve the performance of patch<br />

antennas by introducing air gap between the radiating patch and the<br />

ground plane. Thus, higher bandwidth can be achieved [7]. Circular<br />

polarization is an additional requirement in communication and<br />

it may be achieved either through selection of proper feed<br />

location [8], insertion of suitable slot [9] or through stacking of<br />

patch elements [10].<br />

II. <strong>Antenna</strong> Geometry<br />

A conventional circular patch shown in fig. 1 is modified by<br />

introduction of T shaped slot at the edge. An air stacking of 1<br />

Figure1. Circular microstrip patch antenna<br />

The patch has the diameter of 20 mm. A 50Ω coaxial probe is<br />

used to connect the microstrip patch at coordinates.<br />

Fig. 2(a): Proposed Geometry of <strong>Antenna</strong> (All Dimensions in<br />

mm)<br />

Fig. 2(b): Side View of the Proposed Geometry <strong>with</strong> Coaxial<br />

Feed<br />

www.<strong>iject</strong>.org International Journal of Electronics & Communication Technology 65


IJECT Vo l . 4, Is s u e Sp l - 4, Ap r i l - Ju n e 2013 ISSN : 2230-7109 (Online) | ISSN : 2230-9543 (Print)<br />

The dimensions of T-slot are: vertical arm’s length of 3mm and<br />

vertical arm’s width, horizontal arm’s length & width each of 1mm.<br />

The position of T-slot is (6.5, 0). Thus, impedance-bandwidth of<br />

10.74% can be obtained from the above geometry.<br />

The proposed geometry is designed on glass epoxy FR4 substrate<br />

having thickness h =1.59mm, substrate dielectric constant =4.4,<br />

substrate loss tangent tan δ= 0.024 and relative permeability<br />

=1 <strong>with</strong> an air-gap of 1 mm(foam is used for air-gap). The wider<br />

bandwidth and higher gain (due to air-gap) than the conventional<br />

circular patch <strong>with</strong> simple topology and improvement in the other<br />

antenna radiation parameters are the main advantages of this<br />

geometry. Many simulations are done for optimizing the length;<br />

width and location of the slot and best results are obtained <strong>with</strong><br />

defined length and width of the T-slot. Due to existence of the<br />

T-slot, the current distribution changes and another mode is excited.<br />

Each mode has its own cut-off frequency and thus the proposed<br />

geometry has a new resonant frequency, which is different from<br />

conventional patch resonant frequency.<br />

III. Simulation Results<br />

The simulation results of conventional rectangular patch and<br />

proposed geometry are obtained using IE3D Software [11].<br />

A. Radiation Pattern<br />

A plot through which it is visualized where the antenna transmits<br />

or receives power. The microstrip antenna radiates normal to its<br />

patch surface. So, the elevation pattern for φ= 0 0 and φ= 90 0 are<br />

important for the simulation.<br />

Fig. 4: Computed Elevation Pattern for the Proposed Geometry<br />

The simulated E-plane patterns i.e. the two dimensional patternview<br />

of the geometries is illustrated in fig. 3 and 4. Radiation<br />

patterns are found to be smooth and uniform over the band of<br />

frequencies for both the geometries.<br />

B. Return Loss and Bandwidth<br />

Return Loss is a measure of how much power is delivered from<br />

the source to a load and is measured by S 11<br />

parameters. The range<br />

of frequencies over which the antenna can operate effectively is<br />

characterized by bandwidth. It can be calculated by going 10dB<br />

down in return loss.<br />

Fig. 3: Computed Elevation Pattern for the Conventional<br />

Geometry<br />

Fig. 5: Computed Variation of Return Loss With Frequency for<br />

Conventional Geometry<br />

66 International Journal of Electronics & Communication Technology<br />

www.<strong>iject</strong>.org


ISSN : 2230-7109 (Online) | ISSN : 2230-9543 (Print)<br />

IJECT Vo l . 4, Is s u e Sp l - 4, Ap r i l - Ju n e 2013<br />

Fig. 6: Computed Variation of Return Loss With Frequency for<br />

Proposed Geometry<br />

The variation of return loss <strong>with</strong> frequency is shown in fig. 5 and<br />

6. The conventional patch antenna resonates at frequency of 3.96<br />

GHz <strong>with</strong> -63.53dB return loss and the impedance bandwidth<br />

obtained is 3.41%. The proposed patch antenna has -32.23dB<br />

return loss at resonating frequency of 4.96 GHz and the impedance<br />

bandwidth obtained is 10.74%.<br />

C. Smith Chart<br />

Smith Chart provides the information about the polarization and<br />

the impedance-matching of the radiating patch.<br />

Fig. 8: Variation of Input Impedance With Frequency for Proposed<br />

Geometry<br />

Simulated input impedance variation <strong>with</strong> frequency is shown<br />

in fig. 7 and 8. The circle passes through the centre of the smith<br />

chart represents the impedance match of (49.93-j0.004)Ω for<br />

conventional patch and (51.52+j1.97)Ω for proposed geometry<br />

<strong>with</strong> the coaxial probe and it shows that both geometries have<br />

good impedance matching.<br />

D. Gain<br />

Gain is basically the measure of effectiveness of a directional<br />

antenna as compared to that of a standard non-directional<br />

antenna.<br />

Fig. 7: Variation of Input Impedance With Frequency for<br />

Conventional Geometry<br />

Fig. 9: Computed Variation of Gain With Frequency for<br />

Conventional Geometry<br />

www.<strong>iject</strong>.org International Journal of Electronics & Communication Technology 67


IJECT Vo l . 4, Is s u e Sp l - 4, Ap r i l - Ju n e 2013 ISSN : 2230-7109 (Online) | ISSN : 2230-9543 (Print)<br />

Fig. 10: Computed Variation of Gain With Frequency for Proposed<br />

Geometry<br />

The variation of gain <strong>with</strong> frequency for the conventional and<br />

proposed geometry is shown in fig. 9 and 10. The gain for<br />

conventional geometry is 2.65 dBi and for proposed geometry is<br />

6.12 dBi at resonant frequency; it shows that proposed geometry<br />

has much higher gain over the entire band of frequencies than<br />

conventional geometry.<br />

E. Axial Ratio<br />

This is related <strong>with</strong> quality of circular polarization of an antenna<br />

and axial ratio bandwidth is obtained by calculating the range of<br />

frequencies falling between 0 dB to 3 dB.<br />

Fig. 12: Variation of Axial Ratio With Frequency for Proposed<br />

Geometry<br />

The variation of axial ratio <strong>with</strong> frequency for conventional<br />

patch antenna is shown in fig. 11 it is observed that conventional<br />

geometry is not circularly polarized <strong>with</strong> axial ratio of 51.84dB<br />

at resonant frequency. The axial ratio observed for the proposed<br />

geometry is shown in fig. 12, the geometry is found to be circularly<br />

polarized <strong>with</strong> axial ratio of 0.83dB at resonant frequency and<br />

axial ratio bandwidth of 2.46%.<br />

The comparison between radiation parameters of conventional<br />

patch antenna and proposed geometry is tabulated in Table 1.<br />

Table 1: Comparison of Conventional and Proposed Geometry<br />

Sr.<br />

No.<br />

1.<br />

2.<br />

3.<br />

Parameters<br />

Resonant<br />

Frequency<br />

(GHz)<br />

Return loss<br />

(dB)<br />

Bandwidth<br />

(%)<br />

Conventional<br />

<strong>Patch</strong><br />

3.96 4.96<br />

-63.53 -32.23<br />

3.41 10.74<br />

Proposed <strong>Patch</strong><br />

4. Gain(dBi) 2.65 6.12<br />

4.<br />

Axial Ratio<br />

(dB)<br />

51.84<br />

0.83<br />

(2.46%)<br />

Fig. 11: Variation of Axial Ratio With Frequency for Conventional<br />

Geometry<br />

IV. Conclusion<br />

This paper presents the radiation performance of proposed patch<br />

antenna. The performance of proposed geometry has been compared<br />

<strong>with</strong> conventional geometry. Simulated results indicate that the<br />

antenna exhibits axial ratio bandwidth upto 2.46% by optimizing<br />

the length, width of slots and air gap in proposed antenna geometry.<br />

There is also improvement in impedance bandwidth upto 10.70%.<br />

The radiation patterns in entire bandwidth are identical in nature,<br />

and the direction of maximum radiations over the whole bandwidth<br />

is directed normal to the patch geometry. The obtained results<br />

suggest that proposed antenna may be considered as suitable<br />

candidate for modern wireless communication.<br />

68 International Journal of Electronics & Communication Technology<br />

www.<strong>iject</strong>.org


ISSN : 2230-7109 (Online) | ISSN : 2230-9543 (Print)<br />

IJECT Vo l . 4, Is s u e Sp l - 4, Ap r i l - Ju n e 2013<br />

V. Acknowledgment<br />

The authors would like to thank the authorities of Amity University<br />

Rajasthan and Malaviya National Institute of Technology, Jaipur<br />

for providing the necessary facilities and support.<br />

References<br />

[1] R. Garg, P. Bhartia, I. J. Bhal, A. Ittipiboon,“<strong>Microstrip</strong><br />

<strong>Antenna</strong> Design Book”, Artech House, New York, 2001.<br />

[2] G. Kumar, K.P. Ray,“Broadband <strong>Microstrip</strong> <strong>Antenna</strong>s”,<br />

Artech House, Boston, 2003.<br />

[3] Koray Surmeli, Bahattin Turetken,“U-Slot Stacked <strong>Patch</strong><br />

<strong>Antenna</strong> using High and Low Dielectric Constant Material<br />

Combination in S-Band”, General Assembly and Scientific<br />

Symposium, URSI, August 2011.<br />

[4] Jagtar Singh, A.P Singh, T.S.Kamal,“Design of Circular<br />

<strong>Microstrip</strong> <strong>Antenna</strong> using Artificial Neural Networks”,<br />

Proceedings of the World Congress on Engineering, Vol.<br />

11, U.K, 2011.<br />

[5] Mi-Ra Ryu, Jong-Myung Woo, J. Hu,“Skimmer shaped<br />

Linear <strong>Polarized</strong> <strong>Microstrip</strong> <strong>Antenna</strong>s for Miniaturization”,<br />

International Conference on Advance Communication<br />

Technology, Vol. 1, 4, pp. 758, 2006.<br />

[6] Wu, Jeun Wen, Jui Han Lu,“Slotted Circular <strong>Microstrip</strong> <strong>Patch</strong><br />

<strong>Antenna</strong> for Bandwidth Enhancement”, IEEE Proceeding<br />

Microwave <strong>Antenna</strong>s Propagation, Vol. 2, pp. 272-275,<br />

2003.<br />

[7] Dheeraj Bhardwaj, Komal Sharma, D. Bhatnagar, S.<br />

Sancheti,“Broad Band Parasitically Coupled Concentric Semi<br />

Circular Elliptically Ring <strong>Antenna</strong> Surrounding an Elliptical<br />

<strong>Patch</strong> <strong>with</strong> Air Gap”, 2009 IEEE Applied Electromagnetics<br />

Conference-AEMC, pp. 1-4, 2009.<br />

[8] K.P. Ray, D.D. Krishna,“Compact Dual Band Suspended<br />

Semi-Circular <strong>Microstrip</strong> <strong>Antenna</strong> <strong>with</strong> Half U-slot”,<br />

Microwave Optical Technology Letter No. 48, pp. 2021-<br />

2024, 2007.<br />

[9] Garima, D. Bhatnagar, J.S. Saini, V.K. Saxena, L.M. Joshi,<br />

“Design of Broadband Circular <strong>Antenna</strong> <strong>with</strong> Diamond<br />

Shape Slot”, Indian Journal of Radio & Science Physics,<br />

Vol. 40, pp. 275-281, October 2011.<br />

[10] S. Shekhawat, P. Sekra, D. Bhatnagar, V.K Saxena, J.S Saini,<br />

“Stacked Arrangement of Rectangular <strong>Microstrip</strong> <strong>Patch</strong>es<br />

for <strong>Circularly</strong> <strong>Polarized</strong> Broadband Performance”, IEEE<br />

<strong>Antenna</strong>s Wireless Propagation Letter No. 9, pp. 910–913,<br />

2010.<br />

[11] IE3D software, Release 14.65(Zeland Software Inc.,<br />

Freemont, USA), April 2010.<br />

www.<strong>iject</strong>.org International Journal of Electronics & Communication Technology 69

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