Planar Dipole Antenna with and without Circular Parasitic Element Osman Ayop1, Mohamad Kamal A.Rahim1 and Thelaha Masri1 1 Wireless Communication Centre, Faculty of Electrical Engineering, Universiti teknologi Malaysia, 81310 Skudai Johore Baharu. [email protected], [email protected], [email protected]. Abstract - This paper describe the design of planar Dipole Antenna with Circular Parasitic Element. The comparison between the planar dipole antenna with and without parasitic element has been presented followed by a discussion of the design.. The simulation process was carried out using microwave office and CST software. These antennas were fabricated using inexpensive Fire Retardant-4 (FR4) board, using wet etching techniques. The S11 result shows the operating frequency is between 2.08 GHz and 3.48 GHz for planar dipole antenna with parasitic element. For planar dipole antenna without parasitic element, two ranges of operating frequency is between and 2.1 GHz and 3.08 GHz and another one operational frequency was found at 4.04 GHz and 4.98 GHz. Keywords: planar Dipole Antenna; Circullar Parasitic Element; bandwidth enhancement; Band suppression; 1. Introduction Recent development in wireless communication systems and its application is advancing rapidly not only for commercial but also for military purposes. Wireless technology provides less expensive alternative and a flexible way for communication. In term of frequency, the 2.4 GHz ISM band has become very popular and is now widely used for several wireless communication standards [1]. The planar dipole antenna has been used in this project due to the advantage such as attractive features of low profile, light weight, easy fabrication and conformability to mounting host [2]. The idea of microstrip antenna was first presented in year 1950’s but it only got serious attention in the 1970’s [3]. However microstrip antennas inherently have a narrow bandwidth [4]. In this case, the dipole antenna has been designed to enhance the bandwidth of the microstrip antenna [5]. The dipole can be defined as two straight wire or conductor connecting to the feed line. One of the most commonly used antennas is the half-wavelength (l=λ/2) dipole. Because its radiation resistance is 73 ohms, which is very near the 75-ohm characteristic impedance of some transmission line, its matching to the line is simplified especially at the resonance [6]. Figure 1: Dipole antenna. The electric and magnetic field components of a half-wavelength dipole can be obtained by this formula: π cos cos θ iο e − jkr 2 Hφ ≅ j 2πr sin θ (1) The time-average power density Wav and radiation intensity U can be written, respectively as: 2 π cos cos θ 2 Io 2 ≈ η I o sin 3 θ Wav = η 2 2 2 2 sin θ 8π r 8π r 2 (2) 2 π cos cos θ 2 Io 2 ≈ η I o sin 3 θ 2 U = r Wav = η 2 sin θ 8π 8π 2 r 2 2 (3) The total power radiated Prad can be obtained using this formula: Prad = η Io 8π 2 ∫ 2π 0 π cos cos θ 2 2 dy = η I o cos(2π ) sin θ 8π (4) The dipole antenna has omni directional radiation pattern whose two-dimensional pattern is shown plotted in Figure 2. For the three-dimensional pattern of Figure 3, a 900 angular sector has been removed to 1-4244-1435-0/07/$25.00©2007 IEEE Authorized licensed use limited to: UNIVERSITY TEKNOLOGI MALAYSIA. Downloaded on December 23, 2008 at 02:21 from IEEE Xplore. Restrictions apply. illustrate the figure-eight elevation plane pattern variations. Figure 4: planar dipole antenna without circular parasitic element. Figure 2: 2D Dipole antenna. [2] The rectangular patch size is chosen after the optimization. The length and width of the structure are is 17 mm and 33. The overall size of the antenna is 90 mm x 90 mm with 90 mm x 64 mm ground plane. 2.2 Planar Dipole Antenna with Parasitic Element The microstrip dipole antenna with circular parasitic element has been designed to compare the performance of the antenna with the previous one. Figure 5 shows the microstrip dipole antenna with circular parasitic element. Figure 3: 3D Dipole antenna. [2] 2. The Design and Construction The Dipole Antenna with and without Parasitic element are developed by using inexpensive Fire Retardant-4 (FR4) board which has 1.6 mm-thick substrate with relative permittivity 4.6. The wet etching technique has been used to fabricate the structure after the optimization of the design. 2.1 Planar Dipole Antenna without Parasitic Element The microstrip dipole antenna has been designed due to the larger bandwidth compared to the conventional microstrip antenna design. Figure 4 shows the figure of microstrip dipole antenna with the dimension. Figure 5: Planar dipole antenna with circular parasitic element. The dimensions of the antenna have been shown in the above figure. The unique property of the antenna is the circular shape is used instead using the rectangular shape. Authorized licensed use limited to: UNIVERSITY TEKNOLOGI MALAYSIA. Downloaded on December 23, 2008 at 02:21 from IEEE Xplore. Restrictions apply. 3. Result and Discussion Both antennas have been fabricated and measured. The performances of the structures are evaluated in term of return loss, S11 and radiation pattern. 3.1 Measurement Result of Planar Dipole Antenna without Circular Parasitic Element Figure 6 shows the measurement of return loss result of the planar dipole antenna without circular parasitic element. b) H-plane Figure 7: Radiation pattern of planar dipole antenna without circular parasitic element. 3.2 Measurement Result of Planar Dipole Antenna with Circular Parasitic Element Figure 6: Measured S11 of planar dipole antenna without circular parasitic element. From this result it shows that the operating frequency has been increased between 2.08 GHz and 3.48 GHz. The operating bandwidth is 1.4 GHz compared with the previous result of 0.98 GHz bandwidth. From this result it shows that the operating frequency of the antenna is between 2.1 GHz and 3.08 GHz. The second mode appeared at frequency from 4.04 GHz to 4.98 GHz. Figure 7 below shows the radiation pattern of the microstrip dipole antenna without circular parasitic element at 2.4 GHz for both plane. Figure 8: Measured S11 of planar dipole antenna with circular parasitic element. From figure 8 above, the range of operation frequency of the antenna is from 2.08 GHz to 3.48 GHz which has 1.4 GHz bandwidth. a) E-plane Figure 9 shows that the radiation pattern is very similar with the planar dipole antenna without circular parasitic element. Authorized licensed use limited to: UNIVERSITY TEKNOLOGI MALAYSIA. Downloaded on December 23, 2008 at 02:21 from IEEE Xplore. Restrictions apply. Conclusion The planar dipole antenna with and without circular parasitic element has been presented in this paper. The properties of the antenna such as return loss and radiation pattern has been discussed. It shows that by adding the parasitic elements, the return loss of the antenna has been increased with the same properties of the radiation pattern. a) E-plane Acknowledgement The authors thanks to the Ministry of Higher Education (MOSTI) for supporting the research work, Research Management Centre (RMC) and Wireless Communication Centre, Universiti Teknologi Malaysia (WCC, UTM) for the support of paper presentation. References b) H-plane Figure 9: Radiation pattern of planar dipole antenna with circular parasitic element. 4. Comparison for Planar Dipole antenna with and without Parasitic Element The comparison has been made for both antenna developed in term of S11 and radiation pattern. Referring from figure 10, the bandwidth of the planar dipole antenna with circular parasitic element is wider compared to the planar dipole antenna without circular parasitic element. The second band which appears to the antenna without circular parasitic element is suppressed by adding circular parasitic element at the original structure. [1] M.H. Jamaluddin, M.K.A.Rahim, M.Z.A. Abdul Aziz, ‘Microstrip Dipole Antenna for WLAN application’, 1st International Conference on Computers, Communication and Signal Processing’, 14-16th November 2005, Kuala Lumpur Malaysia [2] M.H. Jamaluddin, M.K.A.Rahim, M.Z.A. Abd Aziz, ‘Microstrip Dipole Antenna analysis of width and length at 2.4 GHz’, Asia Pacific Applied Electromagnetics Conference (APACE 2005), 19-21 December 2005, Johor Bahru Malaysia. [3] M.H. Jamaludin, M.K.A.Rahim, M.Z.A. Abd Aziz, ‘Direct Conversion Receiever for Active Integrated Antenna’, Asia Pacific Applied Electromagnetics Conference (APACE 2005), 1921 December 2005, Johor Bahru Malaysia [4] James, J. R., and P. S. Hall (Eds), Handbook of Microstrip Antennas, Peter Pereginus, London, UK, 1989. [5] TU Zhen, CHEN Guanglin, ZHANG Guangqiu, “The FDTD Analysis Of Two Ultra Wide-band Dipole Antennas,” 2004 4th International Conference on Microwave and Millimeter Wave Technology Proceedings. [6] K.C. Kim and S. Tokumura, “Antenna factor of half-wavelength dipole antennas with Roberts balun”, IEICE Trans, vol. J78-B-II, no. 11, pp. 717-724, Nov 1995. Figure 10: Comparison of measured S11 of planar dipole antenna with and without circular parasitic element. Authorized licensed use limited to: UNIVERSITY TEKNOLOGI MALAYSIA. Downloaded on December 23, 2008 at 02:21 from IEEE Xplore. Restrictions apply.
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