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International Journal of Electronics and Communication
 International Journal of Electronics and Communication Engineering & Technology (IJECET),
Engineering & Technology (IJECET)                                          IJECET
 ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME
ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online)
Volume 1, Number 1, Sep - Oct (2010), pp. 125-130                            ©IAEME
© IAEME, http://www.iaeme.com/ijecet.html


 COMPACT SELF-COMPLEMENTARY ANTENNA FOR X-
                              BAND APPLICATIONS
                                     S A Malipatil
                                 Microwave laboratory
               Department of PG Studies and Research in Applied Electronics
                       Gulbarga University, Gulbarga (Karnataka)
                           E-Mail: malipatilsa@rediffmail.com

                                    S L Mallikarjun
                                 Microwave laboratory
               Department of PG Studies and Research in Applied Electronics
                       Gulbarga University, Gulbarga (Karnataka)
                                      P M Hadalgi
                                 Microwave laboratory
               Department of PG Studies and Research in Applied Electronics
                       Gulbarga University, Gulbarga (Karnataka)
                                    P V Hunagund
                                 Microwave laboratory
               Department of PG Studies and Research in Applied Electronics
                       Gulbarga University, Gulbarga (Karnataka)

ABSTRACT
        Self-complimentary antenna (SCA) on low cost epoxy material is studied.
Dependencies of impedance bandwidth on shapes are clarified by experiments. The self-
complementary antenna impedance matched to a 50               system, utilizing a strip-line feed
is designed and fabricated on a glass epoxy material (Єr = 4.2). The measured return loss
less than -10 dB over a frequency range of 8 – 12 GHz., radiation pattern and gain are
also presented.
Keywords: Self-complementary, glass epoxy, impedance bandwidth, gain, X-band
I. INTRODUCTION
        The self-complementary antenna (SCA) was first proposed by Y. Mushiake [1].
SCA is an arbitrarily shaped antenna which is constituted with a half of an infinitely




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International Journal of Electronics and Communication Engineering & Technology (IJECET),
ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME

extended planar-sheet conductor such that the shape of its complementary structure is
exactly identical with the original structure for the simplest case.
        The type of the SCA is not limited only to the case of a planar antenna, but there
are more general types of structures with various grades of complexity in their structures
such as, the number of terminals, the number of reference planes, and others [2-4].
        In this paper, self-complementary antenna (SCA) fed by strip-line is proposed for
X-band applications. A self-complementary rectangular slot is embedded on the ground
plane, which results into self-complementary structure applied to a finite-sized flat
ground plane is described. Because of the finite-sized ground plane, the antenna can be
applied to small mobile terminals, for which wide bandwidth operation is required. It has
been illustrated that by embedding self-complementary inclined rectangular slot on the
ground plane results into V- shaped self-complementary structure (V-SCA). The optimal
design of this type of antenna can yield an improved impedance bandwidth with
compactness and improvement in radiation properties.
II. ANTENNA DESIGN
        Figure 1 shows the geometry of SCA (θ1 = 00) and V-SCA (θ2 = 100). The design
consists of a rectangular slot etched on the ground plane of the substrate material. The
length and width of the substrate material are L and W. The length and width of the slot
Ls and Ws are taken in term of λ0/2 and λ0/16 respectively, where λ0 is the free space
wavelength in cm. The slot is placed at a distance d from one end of the substrate
material along the center axis of the substrate material, which is in terms of λg/4, where λg
is the guide wavelength in cm. This antenna is energized by strip-line feed, which is
placed at the bottom surface of the substrate material. The length and width of the feed
line are Lf and Wf respectively. The various dimensions of the antenna are listed in table
1.




                                              126
International Journal of Electronics and Communication Engineering & Technology (IJECET),
ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME




                        (a)                                          (b)
                       Figure 1 Geometry of (a) SCA and (b) V-SCA
                    TABLE I - Various dimensions of SCA and V-SCA
                                         L        5.00 cm
                                         W        3.00 cm
                                         Ls       1.60 cm
                                         Ws       0.20 cm
                                         Lf       4.29 cm
                                         Wf       0.84 cm
                                         d        0.57 cm
                                         θ1          00
                                         θ2         100
III. EXPERIMENTAL RESULTS
        The impedance bandwidths over return loss less than –10dB for the proposed
antennas are measured. The measurements are taken on Vector Network Analyzer
(Rohde & Schwarz, German make ZVK Model). The variation of return loss versus
frequency of SCA and V-SCA are shown in Fig. 2. From this graph, the impedance
bandwidth is calculated by using the equation
                                   fH − fL 
                          BW =             ×   100%              (1)
                                   fC 

        Where, fH and fL are the higher and lower cut-off frequencies of the band
respectively when its return loss is -10 dB and fc is the center frequency of band.




                                                 127
International Journal of Electronics and Communication Engineering & Technology (IJECET),
ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME




          Figure 2 Variation of return loss versus frequency of SCA and V-SCA
        From Figure 2 it is clear that the experimental impedance bandwidth (BW1) of
SCA for the angle θ1 resonating at 10.02 GHz is found to be 210 MHz i.e. 1.92 %. The
impedance bandwidth (BW2) of V-SCA for the angle θ2 resonating at 8.97 GHz is found
to be 1920 MHz i.e. 19.73 %, which is 10.30 times more when compared to SCA for the
angle θ1. Further from the graph it is observed that the antenna V-SCA is resonating for
lower frequency resulting in compactness of 11.5 %.
        The X-Y plane co-polar radiation patterns of SCA and V-SCA for the angles θ1and
θ2 are measured at resonating frequencies and are shown in Figure 3. From the figure it is
clear that the antenna V-SCA shows nearly omni-directional radiation pattern.




       Figure 3 Variation of relative power v/s azimuth angle of SCA and V-SSCA


                                              128
International Journal of Electronics and Communication Engineering & Technology (IJECET),
ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME

In order to calculate the gain, the power received (Ps) by the pyramidal horn antenna and
the power received (Pt) by SCA and V-SCA for θ1 and θ2 are measured independently.
With the help of experimental data, the gain of antenna under test (GT) in dB is calculated
using the formula,
                              (GT) dB = (Gs) dB + 10 log (Pt/Ps)         (2)
        Where, Gs is the gain of pyramidal horn antenna. It is seen that the gains of SCA
and V-SCA for θ1 and θ2 are 1.15 dB and 1.09 dB respectively.
        Since V-SCA gives wide impedance bandwidth, the variation of input impedance
is shown in Figure 4. It is seen that the input impedance has a single loop at the centre of
Smith chart that validates its wide single band operation.




                         Figure 4 Input impedance profile of V-SCA
CONCLUSION
        From the detailed study it is clear that, the proposed antennas are quite simple in
design and fabrication and quite good in enhancing the impedance bandwidth with
compact size with improvement in radiation pattern. These antennas are also superior as
they use low cost substrate material. These compact antennas are more suitable where
limited antenna real estate is available and finds application in modern communication
systems.




                                              129
International Journal of Electronics and Communication Engineering & Technology (IJECET),
ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME

Acknowledgment
        We thank the authorities of Department of Science and Technology (DST), Govt,
of India, New Delhi, for sanctioning Vector Network Analyzer under the FIST
Programme to the Department of Applied Electronics, Gulbarga University, Gulbarga.
REFERENCES
[1] Y. Mushiake (1992) “Self-Complementary Antennas”, IEEE Antennas and Prop.
    Magn., Vol. 34, no. 6, pp. 23-29.
[2] Y. Mushiake (2004) “A Report on Japanese Development of Antennas: From the
    Yagi-Uda Antenna to Self-Complementary Antennas”, IEEE Antennas and Prop.
    Magn., Vol. 46, no. 4, pp. 47-60.
[3] Pu. Xu, K. Fujimoto (2003) “L- Shaped Self-Complementary Antenna” Antenna and
    Prop. Soci. Int. Symp. 2003., Vol. 3, pp. 95-98.
[4] Lu Geo et., al., (2008) “A Miniature Quasi-Self-Complementary Antenna for UWB
    Applications”, Microwave Conf. APMC 2008., PP. 1-4.




                                              130

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Compact self complementary antenna for xband applications

  • 1. International Journal of Electronics and Communication International Journal of Electronics and Communication Engineering & Technology (IJECET), Engineering & Technology (IJECET) IJECET ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), pp. 125-130 ©IAEME © IAEME, http://www.iaeme.com/ijecet.html COMPACT SELF-COMPLEMENTARY ANTENNA FOR X- BAND APPLICATIONS S A Malipatil Microwave laboratory Department of PG Studies and Research in Applied Electronics Gulbarga University, Gulbarga (Karnataka) E-Mail: malipatilsa@rediffmail.com S L Mallikarjun Microwave laboratory Department of PG Studies and Research in Applied Electronics Gulbarga University, Gulbarga (Karnataka) P M Hadalgi Microwave laboratory Department of PG Studies and Research in Applied Electronics Gulbarga University, Gulbarga (Karnataka) P V Hunagund Microwave laboratory Department of PG Studies and Research in Applied Electronics Gulbarga University, Gulbarga (Karnataka) ABSTRACT Self-complimentary antenna (SCA) on low cost epoxy material is studied. Dependencies of impedance bandwidth on shapes are clarified by experiments. The self- complementary antenna impedance matched to a 50 system, utilizing a strip-line feed is designed and fabricated on a glass epoxy material (Єr = 4.2). The measured return loss less than -10 dB over a frequency range of 8 – 12 GHz., radiation pattern and gain are also presented. Keywords: Self-complementary, glass epoxy, impedance bandwidth, gain, X-band I. INTRODUCTION The self-complementary antenna (SCA) was first proposed by Y. Mushiake [1]. SCA is an arbitrarily shaped antenna which is constituted with a half of an infinitely 125
  • 2. International Journal of Electronics and Communication Engineering & Technology (IJECET), ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME extended planar-sheet conductor such that the shape of its complementary structure is exactly identical with the original structure for the simplest case. The type of the SCA is not limited only to the case of a planar antenna, but there are more general types of structures with various grades of complexity in their structures such as, the number of terminals, the number of reference planes, and others [2-4]. In this paper, self-complementary antenna (SCA) fed by strip-line is proposed for X-band applications. A self-complementary rectangular slot is embedded on the ground plane, which results into self-complementary structure applied to a finite-sized flat ground plane is described. Because of the finite-sized ground plane, the antenna can be applied to small mobile terminals, for which wide bandwidth operation is required. It has been illustrated that by embedding self-complementary inclined rectangular slot on the ground plane results into V- shaped self-complementary structure (V-SCA). The optimal design of this type of antenna can yield an improved impedance bandwidth with compactness and improvement in radiation properties. II. ANTENNA DESIGN Figure 1 shows the geometry of SCA (θ1 = 00) and V-SCA (θ2 = 100). The design consists of a rectangular slot etched on the ground plane of the substrate material. The length and width of the substrate material are L and W. The length and width of the slot Ls and Ws are taken in term of λ0/2 and λ0/16 respectively, where λ0 is the free space wavelength in cm. The slot is placed at a distance d from one end of the substrate material along the center axis of the substrate material, which is in terms of λg/4, where λg is the guide wavelength in cm. This antenna is energized by strip-line feed, which is placed at the bottom surface of the substrate material. The length and width of the feed line are Lf and Wf respectively. The various dimensions of the antenna are listed in table 1. 126
  • 3. International Journal of Electronics and Communication Engineering & Technology (IJECET), ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME (a) (b) Figure 1 Geometry of (a) SCA and (b) V-SCA TABLE I - Various dimensions of SCA and V-SCA L 5.00 cm W 3.00 cm Ls 1.60 cm Ws 0.20 cm Lf 4.29 cm Wf 0.84 cm d 0.57 cm θ1 00 θ2 100 III. EXPERIMENTAL RESULTS The impedance bandwidths over return loss less than –10dB for the proposed antennas are measured. The measurements are taken on Vector Network Analyzer (Rohde & Schwarz, German make ZVK Model). The variation of return loss versus frequency of SCA and V-SCA are shown in Fig. 2. From this graph, the impedance bandwidth is calculated by using the equation  fH − fL  BW =  × 100% (1)  fC  Where, fH and fL are the higher and lower cut-off frequencies of the band respectively when its return loss is -10 dB and fc is the center frequency of band. 127
  • 4. International Journal of Electronics and Communication Engineering & Technology (IJECET), ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME Figure 2 Variation of return loss versus frequency of SCA and V-SCA From Figure 2 it is clear that the experimental impedance bandwidth (BW1) of SCA for the angle θ1 resonating at 10.02 GHz is found to be 210 MHz i.e. 1.92 %. The impedance bandwidth (BW2) of V-SCA for the angle θ2 resonating at 8.97 GHz is found to be 1920 MHz i.e. 19.73 %, which is 10.30 times more when compared to SCA for the angle θ1. Further from the graph it is observed that the antenna V-SCA is resonating for lower frequency resulting in compactness of 11.5 %. The X-Y plane co-polar radiation patterns of SCA and V-SCA for the angles θ1and θ2 are measured at resonating frequencies and are shown in Figure 3. From the figure it is clear that the antenna V-SCA shows nearly omni-directional radiation pattern. Figure 3 Variation of relative power v/s azimuth angle of SCA and V-SSCA 128
  • 5. International Journal of Electronics and Communication Engineering & Technology (IJECET), ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME In order to calculate the gain, the power received (Ps) by the pyramidal horn antenna and the power received (Pt) by SCA and V-SCA for θ1 and θ2 are measured independently. With the help of experimental data, the gain of antenna under test (GT) in dB is calculated using the formula, (GT) dB = (Gs) dB + 10 log (Pt/Ps) (2) Where, Gs is the gain of pyramidal horn antenna. It is seen that the gains of SCA and V-SCA for θ1 and θ2 are 1.15 dB and 1.09 dB respectively. Since V-SCA gives wide impedance bandwidth, the variation of input impedance is shown in Figure 4. It is seen that the input impedance has a single loop at the centre of Smith chart that validates its wide single band operation. Figure 4 Input impedance profile of V-SCA CONCLUSION From the detailed study it is clear that, the proposed antennas are quite simple in design and fabrication and quite good in enhancing the impedance bandwidth with compact size with improvement in radiation pattern. These antennas are also superior as they use low cost substrate material. These compact antennas are more suitable where limited antenna real estate is available and finds application in modern communication systems. 129
  • 6. International Journal of Electronics and Communication Engineering & Technology (IJECET), ISSN 0976 – 6464(Print), ISSN 0976 – 6472(Online) Volume 1, Number 1, Sep - Oct (2010), © IAEME Acknowledgment We thank the authorities of Department of Science and Technology (DST), Govt, of India, New Delhi, for sanctioning Vector Network Analyzer under the FIST Programme to the Department of Applied Electronics, Gulbarga University, Gulbarga. REFERENCES [1] Y. Mushiake (1992) “Self-Complementary Antennas”, IEEE Antennas and Prop. Magn., Vol. 34, no. 6, pp. 23-29. [2] Y. Mushiake (2004) “A Report on Japanese Development of Antennas: From the Yagi-Uda Antenna to Self-Complementary Antennas”, IEEE Antennas and Prop. Magn., Vol. 46, no. 4, pp. 47-60. [3] Pu. Xu, K. Fujimoto (2003) “L- Shaped Self-Complementary Antenna” Antenna and Prop. Soci. Int. Symp. 2003., Vol. 3, pp. 95-98. [4] Lu Geo et., al., (2008) “A Miniature Quasi-Self-Complementary Antenna for UWB Applications”, Microwave Conf. APMC 2008., PP. 1-4. 130