International Journal of Electromagnetics and Applications
p-ISSN: 2168-5037 e-ISSN: 2168-5045
2013; 3(6): 136-143
doi:10.5923/j.ijea.20130306.02
Dhirgham K. Naji
Department of Electronic and Communications Engineering, College of Engineering, Alnahrain University, Baghdad, Iraq
Correspondence to: Dhirgham K. Naji, Department of Electronic and Communications Engineering, College of Engineering, Alnahrain University, Baghdad, Iraq.
| Email: | ![]() |
Copyright © 2012 Scientific & Academic Publishing. All Rights Reserved.
A design approach for the compact broadband coplanar waveguide (CPW)-fed tapered monopole antenna (TMA) for C-band applications is presented, in this paper. The proposed antenna is composed of a CPW-fed monopole antenna with tapered structures, embedded with symmetric open-ended L-slots, and a tapered shape is cut from the top sides of the CPW-fed ground plane. By loading these structures, the return loss (S11) bandwidth is noticeably increased due to adjacent three resonance modes are generated from the monopole antenna. The designed TMA is simulated by electromagnetic simulator (CST Microwave Studio), with obtained optimal parameters, is demonstrated that
impedance bandwidth is ranging from 3.8 to 8 GHz. The overall dimension of the antenna comes at
This antenna has the advantages of simple configuration, low profile, compactness, and low fabrication cost. The design process and the parametric study of key parameters (taper and slot structures) in producing broadband antenna bandwidth are analyzed and discussed in detail. The simulated results demonstrate that the proposed TMA has good stable omnidirectional radiation patterns, and the peak gain and maximum efficiency over the operating band are 3.4 dBi and 95%, respectively.
Keywords: Broadband, Compact, Coplanar Waveguide, C-band, Tapered Monopole Antenna
Cite this paper: Dhirgham K. Naji, Compact Broadband CPW-fed Taper-shaped Monopole Antenna with L-slots for C-band Applications, International Journal of Electromagnetics and Applications, Vol. 3 No. 6, 2013, pp. 136-143. doi: 10.5923/j.ijea.20130306.02.
and the achieved bandwidth covers 3.8-8 GHz for C-band application.
with relative permittivity,
and the overall occupied area is characterized by substrate length and width,
respectively, i.e.,
The basis of the monopole radiator is a rectangular shape, which has the dimensions of length 
Afterwards, the structure is modified to form a tapered shape of indentation angle
at each side of the monopole width. The width of the CPW feed line is fixed at
and a gap distance of
between the signal strip and the coplanar ground plane of length
is used to achieve
characteristic impedance. The feed line is terminated with a standard SMA connector. The TMA is connected to CPW-strip line and placed at a distance of
from the top of CPW ground plane. An open-ended L-slot, is positioned at the centre of tapered- monopole structures, and characterized by its lengths and widths,
respectively. Finally, a pair of
-tapered structure is cut from the top of two-sided CPW ground plane. The electromagnetic simulation software CST Microwave Studio ver. 2012 is used to design the proposed antenna.![]() | Figure 1. Geometry of the proposed CPW-fed slot antenna for C-band applications. (Unit: mm) |
and the lowest frequency of operation
are given. Then, substrate length
and substrate width
of the antenna are calculated as ![]() | (1) |
![]() | Figure 2. Four improved prototypes of the proposed CPW-fed slot antenna |
is speed of light. Note that the length and width of the antenna structure, according to (1), are equal to half of the effective wavelength at the lower frequency
From (1), one can found that
Afterwards, the CST software is used to sweep each geometric parameter and then the results are fine-tuned until the required resonance frequency with reasonable bandwidth is achieved. As shown in Fig. 3, this design can excite one resonant mode near
ranging from
to
In order to broaden the antenna bandwidth to satisfy C-band operation
Ant 2 is realized by cutting the CPW ground of Ant 1 by tapered structure of angle
It generates two-resonant modes, one at
and is capable of operating over the
frequency range, as noticed in Fig. 3. Thus, the bandwidth is increased without enlarging the size of antenna. It is seen that the lower frequency range
is nearly unaffected, whereas, the upper frequency range
is increased from 6.3 GHz to
when Ant2 is introduced. It needs other modification in Ant2 to increase
toward
the upper range of C-band application. Therefore, Ant3 is proposed for this purpose, which contains other tapered structure of angle
added to the vertical side of the monopole antenna. As seen from Fig. 3, two resonant-modes of
and
are produced and more bandwidth of
ranging from
is achieved compared with Ant2 bandwidth of
It is still that higher frequency range has not satisfied; this leads to introduce Ant4 to perform this requirement. Open-ended L-slots are added to the tapered-monopole structure of Ant3 to increase the perimeter length of the radiating structure which enhances the antenna bandwidth significantly. This can be seen from Fig. 3, where the bandwidth of C-band application is performed which is about of
to
The reason behind that is due to the generation of higher resonant-mode of
in addition to the lower resonant-modes of 4.2 and
that achieved from Ant3. Thus, the Ant 4 (proposed antenna) is capable of satisfying the C-band application, i.e.,
band.![]() | Figure 3. Simulated S11 results for antennas 1-4 (for CPW-fed slot antenna with optimized values of the designed parameters) |
![]() | Figure 4. Simulated results of (a) gain (G) and (b) efficiency of the proposed antenna (Antenna 4) |
and
respectively. The simulated radiation patterns are shown in Figs. 5 and 6. The 3D and 2D patterns are simulated and depicted at three different frequencies (resonant-modes of Ant
Fig. 5 presents 3D farfield gain patterns for the aforementioned three frequencies, as shown, an omnidirectional and stable radiation patterns are achieved for low and middle frequency bands, see Fig. 5(a) and (b). But at high frequency band, Fig. 5(c), nearly omnidirectional with unsymmetrical pattern about xz-plane is obtained. The 2D absolute gain patterns in the yz- or E-plane and xz- or H-plane are seen in Fig. 6 for frequencies, 4.2, 6.2 and 7.80.GHz. It seen that an omnidirectional pattern are sustained in H-plane (xz-plane) over all the frequencies in the C-band. But a figure of 8 is obtained for lower and middle frequencies, Fig. 6(a) and (b), and distorted version of figure 8 is seen for higher frequency in the band, see Fig. 6(c).![]() | Figure 5. Simulated results of 3D farfield gain patterns at for the proposed antenna (Antenna 4) |
![]() | Figure 6. Simulated radiation patterns for the proposed antenna (Ant 4) at (a) 4.2 GHz (b) 6.2 GHz (c) 7.8 GHz |
of the tapered monopole and CPW ground, respectively, and the lengths and widths of L-shaped slot
respectively. These parameters are especially examined to study their influences on impedance bandwidth. All other parameters keep their initial values as seen in Fig. 1.![]() | Figure 7. The simulation results for S11 as affected by parameter (a) (b) ![]() |
of the taper-shaped structures are investigated to find their effects on the antenna performance. We can see that the antenna’s return loss is greatly affected by the ground CPW taper angle
Fig. 7(a), while less effect is observed for the tapered monopole angle
on antenna's return loss, Fig. 7(b). As
the lower resonant-mode is increased from 4.1 to 4.3 GHz with best value
for 4.2 GHz resonant-mode, but higher resonant-mode 7.8 GHz is unaffected for angles less than
and it disappears for angles greater than
. In Fig. 7(b), lower resonant-mode is decreased when
is increases while higher resonant-mode is decreased slightly with increasing in
.
is influences only on higher resonant-mode and not affect on lower resonant-mode. For
the higher frequency band is reduced from
to
and the bandwidth is only
has nearly not changes the return loss when it is varying from
see Fig. 8(b). Also, as seen from Fig. 8(c), the width
is approximately has not affect on the antenna's return loss when it is varying from
to
Finally, as depicted in Fig. 8(d), the width
has little effect on lower resonant-mode, but more effect has been observed at higher resonant-mode, hence, on the bandwidth when it is varying from
It is concluded from the previous discussion that the tapers and L-shaped structures have great influences on the higher-resonant mode and less affect on the lower resonance-mode Also, three out of the six parameters,
and
play an important rule for achieving great enhancement in antenna bandwidth.![]() | Figure 8. ![]() |

has been proposed and simulated using taper and L-shaped structure. The concept of resonant-mode frequencies overlapping technique is used to get wide bandwidth via adding resonant geometrical parts to the antenna. A compact size of TMA structure is obtained from the design process
Additionally, the antenna exhibits a simulated dB return-loss bandwidth of 4.2 GHz ranging from 3.8 to 8 GHz, while maintaining a high efficiency and gain in the order of 95% and 3.4 dBi at the bands of interest. It is therefore well suited for C-band applications. These applications include IEEE 802.11b/g wireless network standards (5.15-5.35 GHz and 5.725-5.825 GHz), communications satellites, satellite radio, weather radar, etc.