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SETIT 2009<br />

5 th International Conference: Sciences <strong>of</strong> Electronic,<br />

Technologies <strong>of</strong> In<strong>for</strong>mation and Telecommunications<br />

March 22-26, 2009 – TUNISIA<br />

<strong>Design</strong> <strong>of</strong> a <strong>Dual</strong>-<strong>Band</strong> <strong>Microstrip</strong> <strong>Patch</strong> <strong>Antenna</strong> <strong>for</strong><br />

<strong>GSM</strong>/<strong>UMTS</strong>/<strong>ISM</strong>/WLAN Operations<br />

Said GHNIMI*, Adnen RAJHI* and Ali GHARSALLAH*<br />

*Unité de recherche Circuits et Systèmes Electroniques Haute Fréquences, Faculté des sciences de Tunis<br />

said.ghnimi@fst.rnu.tn<br />

adnen.Rajhi@esti.rnu.tn<br />

ali.gharsallah@fst.rnu.tn<br />

Abstract: This paper describes the design <strong>of</strong> a dual-frequency antenna <strong>for</strong> <strong>GSM</strong> and <strong>UMTS</strong>/LAN/<strong>ISM</strong> system<br />

applications. A patch antenna with rectangular aperture is designed by using a thick substrate in order to increase the<br />

bandwidth. After this, we have extracted the reflection coefficient <strong>of</strong> the considered antenna excited by a probe feed and<br />

by optimizing the antenna dimensions and the aperture position. The simulation <strong>of</strong> this antenna has been made by<br />

advanced design system (ADS) in the band <strong>of</strong> frequency between 50 Hz and 3.2 GHz, leading to three resonant<br />

frequencies and showing a good impedance bandwidth per<strong>for</strong>mance to cover the required bandwidth <strong>of</strong> the <strong>GSM</strong> (890–<br />

960 MHz), <strong>UMTS</strong> (1920–2170MHz) and WLAN/<strong>ISM</strong> (at 2.45GHz) bands.<br />

Key words: <strong>Microstrip</strong> patch <strong>Antenna</strong>, dual-band, <strong>GSM</strong>, <strong>UMTS</strong>, <strong>ISM</strong> and WLAN.<br />

INTRODUCTION<br />

In the last few years the Global System <strong>for</strong> Mobile<br />

communications (<strong>GSM</strong>) [RAM 03], the Universal<br />

Mobile Telecommunications System (<strong>UMTS</strong>) bands<br />

[HOL 01] [SUR 06] [HUB 00], and one <strong>of</strong> the <strong>ISM</strong><br />

bands is at 2.45 GHz which is also the same band <strong>for</strong><br />

the Wireless Local Area Network (WLAN) system and<br />

Bluetooth applications have been presented in the<br />

published papers [LIU 07] [LEE 97] [MAL 03].<br />

In the literature, several antennas have been<br />

used in a variety <strong>of</strong> applications <strong>for</strong> which new and<br />

more restrictive requirements in the design <strong>of</strong> the<br />

antenna have been introduced. In particular, <strong>for</strong> highprecision<br />

<strong>GSM</strong>, <strong>UMTS</strong> and <strong>ISM</strong>/WLAN applications,<br />

few solutions have been proposed by [CHA 02]<br />

[TUN 02] [CIA 03]. Un<strong>for</strong>tunately, these solutions, it<br />

may easily provide the desired electric characteristics,<br />

but it becomes impractical due to the operational<br />

requirements on size and weight.<br />

The complicated geometry <strong>of</strong> these various<br />

antennas presents the problem at the levels <strong>of</strong> the<br />

realization, which require very sophisticated<br />

equipments and a higher cost <strong>for</strong> the designer, and <strong>for</strong><br />

the integration <strong>of</strong> these antennas in some applications<br />

such as the base station <strong>of</strong> mobile communication.<br />

- 1 -<br />

The proposed antenna presents a simple technique;<br />

indeed, the use <strong>of</strong> a simple substrate <strong>of</strong> low cost and<br />

larger height allows a good impedance matching; then,<br />

it is necessary to sweep on the dimension <strong>of</strong> the<br />

antenna L, W and the aperture size, and the<br />

juxtaposition <strong>of</strong> the feed probe position allows us to<br />

create new resonant frequencies. Once the dimensions<br />

<strong>of</strong> the resonant antenna are determined, the simulated<br />

coefficient <strong>of</strong> reflection S11 is extracted.<br />

Furthermore, in order to satisfy the demanded<br />

precision and reliability, <strong>for</strong> a high per<strong>for</strong>mance<br />

proposed antenna a simple modification on the patch<br />

surface has been introduced.<br />

The organization <strong>of</strong> this paper is as follows,<br />

section 1, the design <strong>for</strong> the proposed dual-band<br />

rectangular patch antenna is presented, in section 2;<br />

we present results and discussions <strong>for</strong> the per<strong>for</strong>mance<br />

<strong>of</strong> the proposed antenna. Section 3, contains<br />

conclusions, and recommendations <strong>for</strong> further studies.<br />

1. <strong>Antenna</strong> <strong>Design</strong><br />

The geometry <strong>of</strong> the proposed dual-band antenna<br />

is based on the microstrip antenna technique which is<br />

the most popular because <strong>of</strong> the ease <strong>of</strong> analysis and<br />

fabrication and having attractive radiation


SETIT2009<br />

characteristics, it consists <strong>of</strong> a rectangular metallic<br />

patch with a rectangular slot mounted on a grounded<br />

substrate as shown in figure 1.<br />

This microstrip antenna is low-pr<strong>of</strong>ile<br />

con<strong>for</strong>mable to planar surfaces, simple and<br />

inexpensive to fabricate using the modern printed<br />

circuit technology and it can be used in many<br />

applications such as the phased array <strong>for</strong> mobile<br />

telecommunication base station. Due to these<br />

advantageous characteristics <strong>of</strong> the proposed<br />

microstrip antenna, further studies and analysis has<br />

been made in this paper.<br />

Figure 1. Geometry <strong>of</strong> the dual-band microstrip<br />

patch antenna.<br />

For its simple structure, the new antenna can<br />

be easily simulated by advanced design system (ADS)<br />

simulator. Some useful guidelines <strong>for</strong> the antenna<br />

design will be discussed as follows.<br />

The structure used in the simulation to<br />

investigate the due to RF pulses is showed in Figure. 1<br />

where a simple microstrip patch antenna was made<br />

with plexy-glass material (εr =2.55), the thickness <strong>of</strong><br />

the patch is assumed negligible and the height h <strong>of</strong> the<br />

substrate is taken equal to 2.5 cm.<br />

The effects <strong>of</strong> the medium and the fringing<br />

fields at each end <strong>of</strong> the patch are accounted <strong>for</strong> by the<br />

effective relative dielectric constant, εeff, and the edge<br />

extension, ∆L, being the effective length to which the<br />

fields fringe at each end <strong>of</strong> the patch. The following<br />

effective dielectric constant <strong>for</strong>mula proposed is used<br />

in equation 1<br />

1<br />

−<br />

2<br />

ε r + 1 ε r −1<br />

h<br />

ε eff = + ( 1+<br />

12 ) (1)<br />

2 2 W<br />

- 2 -<br />

With<br />

∆L<br />

=<br />

h<br />

And<br />

0,<br />

412<br />

( ε<br />

( ε<br />

r<br />

eff<br />

eff<br />

W<br />

+ 0,<br />

3)(<br />

+ 0,<br />

264)<br />

h<br />

W<br />

− 0,<br />

258)(<br />

+ 0,<br />

8)<br />

h<br />

r<br />

eff<br />

(2)<br />

λ C c0<br />

L = = =<br />

(3)<br />

2 2 f 2 f ε<br />

In general, the resonant frequency <strong>of</strong> rectangular<br />

patch antennas is calculated by using resonant length<br />

transmission line or cavity models, together with<br />

equations <strong>for</strong> the effective dielectric constant and edge<br />

extension from the literature. The resonant frequency<br />

fmn <strong>of</strong> a rectangular patch <strong>of</strong> width W and length L,<br />

both comparable to λs /2, where λs is the wavelength<br />

in the substrate, is given by<br />

f<br />

mn<br />

2<br />

2<br />

c ⎡⎛<br />

⎞ ⎤<br />

0 m ⎛ n ⎞<br />

= ⎢<br />

⎜<br />

⎟ +<br />

⎜<br />

⎟ ⎥<br />

2 ε ⎢⎣<br />

⎝ L<br />

eff e ⎠ ⎝We<br />

⎠ ⎥⎦<br />

(4)<br />

Where εeff is the effective relative dielectric<br />

constant <strong>for</strong> the patch, m and n take integer values,<br />

and Le and We are the effective dimensions.<br />

L e<br />

The effective length Le can be defined as follows:<br />

= L + 2 ∆L<br />

(5)<br />

In order to determine the resonant frequency, the<br />

band <strong>of</strong> use <strong>of</strong> this antenna is defined by:<br />

Fmax<br />

− Finf<br />

B(%)<br />

= 100<br />

(6)<br />

F<br />

r<br />

The dimensions <strong>of</strong> the proposed patch are the<br />

width W= 8cm and the length L=8.55 cm, with a<br />

copper plane on one side; in the patch, a slot is<br />

designed with a length equal to y2-y1 = 4cm and a<br />

width x0 = 0.4cm, the distance between the probe feed<br />

and the slot is d=y1-y0. The coaxial feed was excited<br />

by RF source with impedance <strong>of</strong> 50 Ohms, and the<br />

frequency band <strong>of</strong> analysis ranges the antenna from<br />

electrically short at the lowest frequency to electrically<br />

long at the highest frequency.


SETIT2009<br />

2. Results and discussion<br />

A prototype <strong>of</strong> the antenna has been tested by<br />

ADS simulator, with the above given geometrical<br />

dimensions <strong>of</strong> the patch. The simulation returns loss <strong>of</strong><br />

this antenna is presented in figure 2 <strong>for</strong> three different<br />

distances between the probe feed and the slot edge<br />

(d1=0.01mm d2=1cm, d3=2cm).<br />

Return loss[dB]<br />

0<br />

-5<br />

-10<br />

-15<br />

-20<br />

-25<br />

-30<br />

-35<br />

-40<br />

-45<br />

<strong>GSM</strong> band<br />

S11<br />

d1<br />

d2<br />

d3<br />

<strong>UMTS</strong> band<br />

0.5 1 1.5 2 2.5 3<br />

x 10 9<br />

Frequency[Hz]<br />

Figure 2. Comparisons <strong>of</strong> the simulated return loss <strong>of</strong><br />

the microstrip patch antenna <strong>for</strong> different distances<br />

(d1=0.01mm d2=1cm, d3=2cm).<br />

From this simulation we found dual bands, the first<br />

is around a resonant frequency Fr1 and the second<br />

band can be considered as around two resonant<br />

frequencies (Fr2, Fr3), and it demonstrates that a<br />

good input match has been obtained <strong>for</strong> both the<br />

<strong>GSM</strong>/<strong>UMTS</strong> bands and LAN/<strong>ISM</strong> operations. The<br />

optimal proposed antenna is <strong>for</strong> d2=1cm which covers<br />

the required bandwidth respectively <strong>of</strong> the <strong>GSM</strong> 900,<br />

<strong>UMTS</strong> 2000 bands and <strong>ISM</strong>/WLAN 2450 operations.<br />

For <strong>GSM</strong> 900, a wide operating frequency range <strong>of</strong><br />

890 to 995 MHz is obtained, and the impedance<br />

bandwidth determined from -10 dB return loss can<br />

reach 105 MHz (or 11.37 % referenced to 923 MHz).<br />

For <strong>UMTS</strong> 2000, a much wider operating frequency<br />

range <strong>of</strong> 1900 to 3100 MHz can be obtained, and the<br />

impedance bandwidth determined from -10 dB return<br />

loss can even reach 1200 MHz (or 55.88 % referenced<br />

to 2150 MHz).<br />

The simulation results are summarized in the<br />

table’s 1-3.<br />

Type<br />

d’antenne<br />

Central<br />

d1 d2 d3<br />

frequency<br />

Fr1GHz<br />

0.921 0.923 0.921<br />

BP [%] 10.74 11.37 9.66<br />

Table 1. <strong>Band</strong>width around Fr1<br />

- 3 -<br />

Table 1, present the bandwidth around the first<br />

Fr1 resonance frequency and it is noted that the<br />

resonant frequency Fr1 and the bandwidth are almost<br />

the same one <strong>for</strong> the different distances d.<br />

Table 2. <strong>Band</strong>width around Fr2<br />

Table 3. <strong>Band</strong>width around Fr3<br />

Table 2 and Table 3, present respectively the<br />

bandwidth around the resonance Fr2 and Fr3<br />

frequency, and it is noted that the bandwidth depends<br />

on the distance d. Indeed, one notes <strong>for</strong> d= 1cm the<br />

microstrip patch antenna present a large bandwidth<br />

and more per<strong>for</strong>mance around resonance frequency.<br />

By analyzing the ADS Simulation results <strong>of</strong> the<br />

reflection coefficient <strong>of</strong> the proposed antenna, we can<br />

conclude that the antenna has three resonant<br />

frequencies (Fr1, Fr2, and Fr3); and <strong>for</strong> the different<br />

distances, the frequency Fr1 is almost the same, but<br />

the other frequencies Fr2 and Fr3 changes by<br />

changing the distance d.<br />

The resonant frequency Fr1 given by (7) can be<br />

calculated from the fundamental TM10 mode <strong>of</strong> the<br />

patch antenna with the dimensions (W = 8cm, L =<br />

8.55 cm), to intend <strong>GSM</strong> band.<br />

F<br />

r1<br />

Type<br />

d’antenne<br />

Central<br />

d1 d2 d3<br />

frequency<br />

Fr2GHz<br />

2.25 2.15 2.16<br />

BP [%] 47.55 55.88 28.37<br />

Type<br />

d’antenne<br />

Central<br />

d1 d2 d3<br />

frequency<br />

Fr3GHz<br />

2.74 2.97 2.85<br />

BP [%] 39.05 40.4 17.54<br />

c0<br />

= f10<br />

=<br />

(7)<br />

2L<br />

ε<br />

e<br />

eff<br />

In order to investigate the dependence at the<br />

second resonant frequency Fr2 and at the third<br />

resonant frequency Fr3 according to the different<br />

values <strong>of</strong> d which represent the distance between the<br />

probe feed and the slot, figure.3 and figure.4 are<br />

presented to explain this dependence.


SETIT2009<br />

Fr2[GHz]<br />

Fr3[GHz]<br />

2.28<br />

2.26<br />

2.24<br />

2.22<br />

2.2<br />

2.18<br />

2.16<br />

2.14<br />

0 0.2 0.4 0.6 0.8 1<br />

d[cm]<br />

1.2 1.4 1.6 1.8 2<br />

3<br />

2.95<br />

2.9<br />

2.85<br />

2.8<br />

2.75<br />

Figure 3. Effect <strong>of</strong> the distance d on resonance<br />

frequency Fr2<br />

2.7<br />

0 0.2 0.4 0.6 0.8 1<br />

d[cm]<br />

1.2 1.4 1.6 1.8 2<br />

Figure 4. Effect <strong>of</strong> the distance d on resonance<br />

frequency Fr3<br />

Figure.3 and Figure.4 show how the both<br />

resonances frequencies Fr2 and Fr3, depend<br />

respectively from the distance d between the slot and<br />

the probe feed, indeed, these variations <strong>of</strong> Fr2 and Fr3<br />

have inverse behaviors if Fr2 increases then Fr3<br />

decreases and vice versa.<br />

3. Conclusion<br />

The main quality <strong>of</strong> the proposed antenna is that it<br />

allows an effective design maintaining all the<br />

advantages <strong>of</strong> microstrip antennas in terms <strong>of</strong> size,<br />

weight and easy manufacturing. Moreover, this<br />

antenna has a good effectiveness on the totality <strong>of</strong> the<br />

three covered respectively, <strong>GSM</strong>, <strong>UMTS</strong> and<br />

WLAN/<strong>ISM</strong> frequency bands. This work has to be<br />

studied further to have more precise expressions <strong>for</strong><br />

- 4 -<br />

the dependence <strong>of</strong> Fr2 and Fr3 with the distance d<br />

between the slot and the feed probe.<br />

REFERENCES<br />

[RAM 03] Rammal, M.; Abou Chahine, S.; Fadlallah, N,<br />

“An improved FDTD design <strong>of</strong> a wideband <strong>GSM</strong> patch<br />

antenna”, Proceedings <strong>of</strong> the Twentieth National Radio<br />

Science Conference, March 2003, pp.B17 - 1-5.<br />

[HOL 01] H. Holma and A. Toskala, “WCDMA <strong>for</strong> <strong>UMTS</strong>:<br />

Radio Access <strong>for</strong> Third Generation Mobile<br />

Communications”, John Wiley & Sons, New York,<br />

2001.<br />

[SUR 06] E. Surducan, D.S.Iancu, V.Surducan, J.Glossner,<br />

“<strong>Microstrip</strong> composite antenna <strong>for</strong> multiple<br />

Communication protocols”, International Journal <strong>of</strong><br />

Microwave and Optical Technology, (IJMOT 2006-5-30)<br />

Vol-I-No.2, 2006, pp.772-775, ISSN 1553-0396.<br />

[HUB 00] J.F. Hubner, D. Weiler, H. Brand, “<strong>UMTS</strong>, the<br />

Mobile Multimedia Vision <strong>for</strong> IMT-2000: A Focus on<br />

Standardization”, IEEE Communication Magazine,<br />

September 2000, pp. 129-136.<br />

[LIU 07] Juan Liu, Jing Xia, Gang Wang,“A <strong>Dual</strong>-<strong>Band</strong><br />

<strong>Microstrip</strong>-Fed Bow-Tie <strong>Antenna</strong> <strong>for</strong> <strong>GSM</strong>/CDMA and<br />

3G/WLAN”, IEEE 2007 International Symposium on<br />

Microwave, <strong>Antenna</strong>, Propagation, and EMC<br />

Technologies For Wireless Communications, Aug. 2007,<br />

pp.504-507.<br />

[LEE 97] K.F. Lee, et al., “Experimental and Simulation<br />

Studies <strong>of</strong> the Coaxially Fed U-slot Rectangular <strong>Patch</strong><br />

<strong>Antenna</strong> ”, IEE Proceedings- Microwave <strong>Antenna</strong>s and<br />

Propagation, Vol. 144, No. 5, 1997, pp. 354–358.<br />

[MAL 03] Malisuwan, S.; Charoenwattanapom, M.;<br />

Huvanandana, S.; Rosesukon, K., “<strong>Design</strong> <strong>of</strong> <strong>Microstrip</strong><br />

<strong>Antenna</strong> <strong>for</strong> Bluetooth and WAN Applications y<br />

Applying Modified Smithchart Representation”, IEEE<br />

2003 Asia-Paclfc Conference on Applied<br />

Electromagnetics (APACE 2003), Malaysia, pp. 38-41.<br />

[CHA 02] CHANG, F.S., YEH, S.H., and WONG, K.L.:<br />

“Planar monopole in wrapped structure <strong>for</strong> low-pr<strong>of</strong>ile<br />

<strong>GSM</strong>/DCS mobile phone”, Electron. Lett, 2002, 38,<br />

(11), pp. 499–500.<br />

[TUN 02] H. C. Tung and K. L. Wong, “<strong>Dual</strong>-<strong>Band</strong><br />

Inverted-L Monopole <strong>Antenna</strong> <strong>for</strong> <strong>GSM</strong>/DCS Mobile<br />

Phone,” in 2002 IEEE <strong>Antenna</strong>s Propagat. Soc. Int.<br />

Symp. Dig., San Antonio, Texas, USA, vol. 3, pp. 30-33.


SETIT2009<br />

[CIA 03] P. CIAIS, R. STARAJ, G. KOSSIAVAS, C.<br />

LUXEY, “Antenne miniature quadri-bande<br />

<strong>GSM</strong>/DCS/PCS/<strong>UMTS</strong> ”, 13émes Journées Nationales<br />

Microondes, LILLE, mai 2003 , pp21-23.<br />

- 5 -

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