Jurnal Teknologi DESIGN OF SIERPINSKI GASKET FRACTAL ANTENNA WITH SLITS FOR MULTIBAND APPLICATION. Full Paper

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Jurnal Teknologi DESIGN OF SIERPINSKI GASKET FRACTAL ANTENNA WITH SLITS FOR MULTIBAND APPLICATION Mohamad Hafize Ramli a *, Mohamad Zoinol Abidin Abd. Aziz a, Mohd Azlishah Othman a, Nornikman Hassan a, Muhammad Syafiq Noor Azizi a, Siti Nurfarhanah Azizul Azlan a, Abdul Halim Dahalan b, Hamzah Asyrani Sulaiman c a Centre for Telecommunication Research and Innovation (CeTRI), Faculty of Electronics and Computer Engineering, Universiti Teknikal Malaysia Melaka (UTeM), 76100 Durian Tunggal, Melaka, Malaysia b Faculty of Engineering Technology, Universiti Teknikal Malaysia Melaka (UTeM), 76100 Durian Tunggal, Melaka, Malaysia c Faculty of Information and Communication Technology, Universiti Teknikal Malaysia Melaka (UTeM), 76100 Durian Tunggal, Melaka, Malaysia Full Paper Article history Received 1 August 2015 Received in revised form 14 December 2015 Accepted 19 January 2016 *Corresponding author hafizeramli@utem.edu.my Graphical abstract Abstract There is highly demand of antenna with these characteristics: compact size, low profile and multiband or broadband but at the same time have to maintain antenna parameters. This paper focuses on design of Sierpinski Gasket Fractal Antenna (SGFA) with slits for multiband application.two methods are applied to this antenna to improve its performance. The first method is by adding two slits on the fractal antenna. The second method is by increasing the number of s of the fractal antenna. These methods can improve the return loss and gain of the antenna. The simulation of the designed antenna is carried out by using Computer Simulation Technology (CST) software. The simulated return loss of SGFA with slit is about -20.1 db and -11.64 db compare with SGFA without slit -19.25 db and -12.27 db at 2.4 GHZ and 5 GHz. While, the gain also increase when slit is added to SGFA. The simulated and measured of antenna parameter is well compared. Keywords: Sierpinski gasket fractal antenna, slits, return loss,gain, 2016 Penerbit UTM Press. All rights reserved 1.0 INTRODUCTION In today world of wireless communications, there has been an increasing need for more compact and portable communications systems. Just as the size of circuitry has evolved to transceivers on a single chip, there is also a need to evolve antenna design to minimize the design. In the study of antennas, fractal antenna theory is a new area in antenna design technology. A fractal antenna is created using fractal geometry, a self-similar pattern built from the repetition of a simple shape [1]. The inherent qualities of fractals enable the production of high performance antennas that are typically 50 to 75 percent smaller than traditional antennas [1-2]. Several fractal antennas have been proposed to obtain multi-band frequency operation. A dual band wireless device PCB fractal monopole antenna which can operate on WLAN or Bluetooth applications. The modified Sierpinski gasket is an efficient radiator with the ability to handle both the 2.4 and 5.2 GHz ISM bands without a matching network. The size of 78: 5 8 (2016) 123 128 www.jurnalteknologi.utm.my eissn 2180 3722

124 Mohamad Hafize Ramli et al. / JurnalTeknologi (Sciences & Engineering) 78: 5 8 (2016) 123 128 antenna is reduced by controlling the space factor between the first two resonances [3]. Then, in [4] a modified Sierpinski fractal patch antenna with small triangles is drawn outside on three sides of each equilateral triangle to increase the radiating area.while, in [5] the SGFA has been designed and fabricated with defected ground structure (DGS) with center frequency at 5.8 GHz. A slot was used as a DGS. DGS was introduced in the design to increase the bandwidth as well as to further miniaturize the size of the antenna. The SGFA with slit has been reported in [6] about a design of dual band triangular fractal antenna with slits for wireless applications. The slits are made at the three corners of the triangular patch. Ground plane is located on the bottom side of the substrate. Port is to be placed in the antenna in order to achieve the circular polarization. In this paper, a design of Sierpinski Gasket Fractal Antenna (SGFA) with slits for multiband application has been proposed. The slits are placed near to the feed line to have better return loss. The number of is increased up to fourth s to lower the resonance frequency. The designed antenna can operate on WLAN (IEEE 802.11a) and Bluetooth (IEEE 802.15.1) applications. Table 2 The dimension of the SGFA with/out slit (calculated and optimized) Symbol Description Value (mm) TH Triangle height 62.355 TS Triangle side length for 0 72 TS1 Triangle side length for 1 36 TS2 Triangle side length for 2 18 TS3 Triangle side length for 3 9 TS4 Triangle side length for 4 4.5 Lg Substrate length 85 Wg Substrate width 89.6 h Substrate thickness 1.6 Wf Feed line width 4.5 Lf Feed line length 3.89 SL Slit length 2.5 SW Slit width 1 L1 Length between triangle 4.8 patch and substrate W1 Width between triangle patch 4.8 and substrate t Copper thickness 0.035 2.0 ANTENNA DESIGN Table 1 shows the substrate specification of proposed antenna. The proposed antenna is a broadband operation. The return loss of the antenna must be below -10dB to make sure the proposed antenna can achieve at least 90% matching efficiency [5]. The antenna is designed by using a FR4 epoxy dielectric substrate with dielectric constant, ε r = 4.4, tangent loss, tan δ = 0.019 and the thickness, t of substrate, h = 1.6mm.While, Table 2 shows the dimension of the SGFA with/out slit. The front view of SGFA with no slit is shown in Figure 1. The yellow region represents the copper layer of antenna while the blue region represents the substrate of the antenna. Then, Figure 2 shows the front view of SGFA with slit. Next, Figure 3 and 4 shows the bottom and side view of the antenna. Table 1 Substrate specification Substrate FR4 Relative permittivity,ε r 4.4 Tangent loss, δ 0.019 Substrate thickness, h 1.6mm Copper thickness, t 0.035mm Figure 1 The front view of SGFA structure with no slit

125 Mohamad Hafize Ramli et al. / JurnalTeknologi (Sciences & Engineering) 78: 5 8 (2016) 123 128 ε r is the relative permittivity of substrate f r is the resonant frequency c is the speed of light in vacuum The triangle side length for 1 st, 2 nd, 3 rd, and 4 th is calculated by using equation (2). T si = T s i = 2i 1,2,3,4 (2) The next resonant frequency can be calculated by using equation (3) [4], [7], [8]. Figure 2 The front view of SGFA structure with slit f r (0.15345 + 0.3ρx) c h e ( 1 n ) for n = 0 0.26 c δ n for n > 0 h e S e = S + t(ε r ) 0.5 is the effective side length of the largest gasket h e = 3S e is the effective height of the largest gasket 2 (3) The substrate length and width are calculated by using equation (4) and equation (5) [9]. Figure 3 The bottom view of SGFA structure with slit L g = T H + 6h (4) (5) W g = T S + 6h (4) Figure 4 The side view of SGFA structure with slit The antenna design process starts with calculation of side length of triangle [4], [7], [8]. The side length of the triangle, TS is calculated by using equation (1). T s = 1 (0.3069 + 0.68ρx) c 3 f r ( 1 n ) 1 for n = 0 ε r 0.52 c 3 f r δ n 1 ε r for n > 0 (1) The slit length is obtained through parametric study while the slit width is assumed to be 1mm [10], [11]. The feed line width is calculated by using transmission line modal in equation (6) [13]. (5) = h k+1 is the ratio of height of gasket in the (k+1)th h k to that in the kth. δ = 1 is the scale factor n is the band number ρ = 0.230735 0, k = 0 x = 1, k > 0 t is the thickness of substrate W f = h 8e A e 2A 2 for W f h < 2 2 [B 1 ln(2b 1) + ε r 1 [ln(b 1) + 0.39 0.61 ]] for W f π 2ε r ε r A = Z τ 60 ε r + 1 + ε r 1 0.11 (0.23 + ) 2 ε r + 1 ε r 377π B = 2Z τ ε r h > 2 (6)

126 Mohamad Hafize Ramli et al. / JurnalTeknologi (Sciences & Engineering) 78: 5 8 (2016) 123 128 The feed line length is calculated by using quarter wave transformer technique in equation (7) [12]. Z τ = Z o Z in Z in is the reference impedance simulated from CST Z o is the characteristic impedance (7) simulation and measurement of SGFA. The measured return loss at 2.4GHz and 5GHz are -11.466dB and - 8.3543dB respectively. The measured return loss and gain is decrease and not shows a good responsecompare the simulation result. The measured return loss at 5GHz does not less than -10dB. This might be due to human error during the antenna fabrication process. 3.0 RESULT AND DISCUSSION These sections show the several performance of the Sierpinski gasket fractal antenna (SGFA) with slit.parametric study on the slit length is conducted in order to get the optimum result for the return loss. The variation of slit length has been selected from 1.2 mm until 2.4 mm. Although there is no significant changes, but 1.8mm of slit length give optimize return loss for this antenna. The return loss at 2.41GHz is -20.1dB while the return loss at 5GHz is -11.6dB. Figure 5 shows the simulatedreturn loss for SGFA with/out slit. While, Table 3 shows the comparison of antenna parameter between SGFA with/out slit. There are no significant differences by adding slit to the fractal antenna. There are certain parameter like bandwidth has become narrow after adding slit. Only the return loss and gain at 2.4GHz is improved. The designed antenna has 2.49dB of gain at 2.4GHz and 3.75dB of gain at 5GHz respectively. Figure 6 Comparison return loss between simulation and measurement Table 4 Comparison of antenna parameter between simulation and measurement Parameters Simulation Measurement Frequency 2.4GHz 5GHz 2.4GHz 5GHz Return loss (db) -20.1-11.64-11.466-8.3543 Gain (db) 2.49 3.74 1.87 2.29 Figure 7and 9 shows the 2D radiation pattern for SGFA with slit for phi=00 and phi=900at 2.4 GHz and 5 GHz. The radiation pattern at 5 GHz has bigger main lobe compare to 2.4 GHz for phi=00. Both of these also have back lobes. While, the radiation pattern at 2.4GHz is nearly omnidirectional pattern. The radiation pattern at 5GHz has two main lobes and a side lobe. Figure 8 and 10 show the 3D radiation pattern for SGFA with slit at 2.4 GHz and 5 GHz. It s show that radiation mostly concentrates in front of the SGFA area. Figure 5 Simulated return loss for SGFA with/out slit Table 3 Comparison of antenna parameter between SGFA with/out slit. Parameters With slit Without slit Frequency 2.28-4.68-2.29-4.69-5.13 range (GHz) 2.54 5.07 2.56 Bandwidth 0.26 0.39 0.27 0.44 (GHz) Return loss -20.1-11.64-19.25-12.27 (db) Gain (db) 2.49 3.74 2.27 3.52 Efficiency (db) -2.25-1.87-2.21-1.84 Figure 6 shows the comparison of return loss between simulation and measurement. While, Table 4 shows the comparison of antenna parameters (a)

127 Mohamad Hafize Ramli et al. / JurnalTeknologi (Sciences & Engineering) 78: 5 8 (2016) 123 128 (b) Figure 7 2D radiation pattern for SGFA with slit for phi=0 0 ; (a) 2.4GHz and (b) 5GHz Figure 10 3D radiation pattern for SGFA with slit at 5 GHz Figure 11 and 12 show the surface current distribution of SGFA with slit at resonant frequency of 2.4 GHz and 5 GHz. The red arrow show the significant high surface current distribution compare with the green arrow. While Figure 13 shows the fabricated antenna of SGFA with slits. Figure 8 3D radiation pattern for SGFA with slit at 2.4 GHz (a) (b) Figure 11 Surface current distribution of SGFA with slit at 2.4 GHz. Figure 9 2D radiation pattern for SGFA with slit for phi=90 0 ; (a) 2.4GHz and (b) 5GHz

128 Mohamad Hafize Ramli et al. / JurnalTeknologi (Sciences & Engineering) 78: 5 8 (2016) 123 128 4.0 CONCLUSIONS As a conclusion, the Sierpinski Gasket fractal antenna with slits for multiband applications has been designed and fabricated. The simulation results showed that the designed antenna covered the frequencies from 2.28GHz to 2.54GHz and 4.68GHz to 5.07GHz. Hence, the designed antenna can be used for multiband applications. The measured antenna gain does not achieve as desired. Others substrate like Roger 5880 can be used to reduce the antenna loss because FR4 has higher loss compared to others substrate. References Figure 12 Surface current distribution of SGFA with slits at 5 GHz. Figure 13 Fabricated antenna of SGFA with slits [1] Manjibhai, D. A.,Prajapati, J. C.,Barasara, D. J. 2012. An Overview of Fractal Geometries and Antenna, International Journal of Engineering and Science. 1(2): 1-4. [2] Hu, Z, Wan, G., Sun, C.J., Zhao, H. L. 2009. Design of Modified Sierpinski Fractal Antenna for Multiband Application, Microwave, Antenna, Propagation and EMC Technologies for Wireless Communications. 655-658. [3] Krzysztofik, W. J. 2009. Fractal Antenna for WLAN/Bluetooth Multiple-Bands Applications, 3 rd European Conference. 2407-2410. [4] Singh, M. Kumar, N.,Diwari, S., Kala, P. 2013. Bandwidth Enhancement using Small Triangles on Sierpinski Fractal, Signal Processing and Communication (ICSC). 86 91. [5] Ismail, K.,Ishak, S.H.2012. Sierpinski Gasket Fractal Antenna with Defected Ground Structure, ICT Convergence.441-446. [6] Renuga, M. D., Dharani, K. R.,Pavithra, D., Poongodi, C. 2014. Design of Dual Band Triangular Fractal Antenna with Slits for Wireless Applications. International Journal of Scientific Research in Computer Science Applications and Management Studies. 3(2): 23-30. [7] Mishra, R. K.,Ghatak R., Podder,D. 2008. Design Formula for Sierpinski Gasket Pre-Fractal Planar-Monopole Antennas, Antennas and Propagation Magazine. 50(3): 104 107. [8] Saluja1, N., Khanna, R. 2012. A Novel Method to Improve Current Density in Multiband Triangular Fractal Antenna. Elektronika IR Elektrotechnika.18: 41 44. [9] Shrestha, S.,Lee, S. R., Choi, D. Y. 2014. A New Fractal-Based Miniaturized Dual Band Patch Antenna for RF Energy Harvesting, International Journal of Antennas and Propagation. 3(1): 1-6. [10] Wong, K. L.,Fang, S. T.,Lu, J. H. 1998. Dual Frequency Equilateral Triangular Microstrip Antenna With A Slit, John Wiley & Sons, Inc. Microwave OptTechnol Lett. 348-350. [11] Surjati,I.,Rahardjo,E. K., 2012. Dual Frequency Operation of Equilateral Triangulat Microstrip Antenna Using Microstrip Feed Line, International Journal of Technology and Engineering System. 3: 12-16. [12] Pozar,D. M. 2012. Microwave Engineering. 4rd ed., John Wiley & Sons, lnc. 148-149.