KnE Social Sciences | 3rd UNJ International Conference on Technical and Vocational Education and Training 2018 (3rd ICTVET 2018) | pages: 498–506

, , and

1. Introduction

Ground Penetrating Radar (GPR) is a technology that has been developed within 15-20 years ago. The advancement involves theories, techniques, technology and also applications range. GPR is an imaging tool that uses electromagnetic waves to observe underground material. At the beginning of its emergence, GPR technology is used to detect natural materials, but as the theory and technique progress, GPR also is also used to detect unnatural materials such as asphalt, concrete, and even bridge structures. Each material that we want to detect has different GPR specifications due to different permittivity value. Simply talk, the GPR works by counting the amount of reflection and electromagnetic waves that fired on the surface [1].

There are two important parts in GPR: the antenna and the processing system to process a received / reflected signal. This paper focuses on the antenna used by GPR: Vivaldi antenna. Vivaldi antenna was first used by Gibson in 1979 with very wide bandwidth characteristics and directional radiation patterns [2]. Theoretically, Vivaldi antennas have infinite bandwidth, high gain, and linear polarization [3]. Figure 1 shows the concept of a Vivaldi antenna in the front view.

Figure 1

Vivaldi Antenna.


Dimension parameters of Vivaldi Antenna are antenna length (PA), antenna width (LA), tapered length (TL), tapered rate (r), slot-line length (sL), back-wall offset (bwo) and opening mouth (MO).The Vivaldi antenna included in the Exponential Tapered Slot Antenna (TSA) type.

2. Methods and Equipment


The development of the Vivaldi antenna on this paper begins by determining some antenna parameters to specify the initial antenna. The next step is making antenna modeling by using antenna simulation software based on parameters specified in the antenna dimension parameters. Antenna simulation is used to find out whether the antenna model meets antenna specifications for the Ground Penetrating Radar (GPR). After all antenna parameters are specified and simulated, the parameters are compared to the desired specification (frequency, return loss, VSWR). Frequency that use on GPR for non-destructive testing application is 700 – 2000 MHz. Our target for antenna frequency is 1 – 2 GHz, so that the antenna bandwidth is 1 GHz. If simulation result shows that antenna does not meet the specification yet, optimization is carried out. Optimization is done to achieve the specifications needed by learning various things, other literacy and also trial and error. Optimization is done by changing the values of the antenna dimension parameters. Each antenna dimension parameter has an effect for bandwidth antenna performance during this research period. Thus connecting between antenna width parameter and bandwidth of the Vivaldi antenna becomes one of the data results in this research.

The length (PA) and width (LA) of the antenna is determined by equation (1).


where PA is an antenna length, LA is an antenna width, c is a speed of light, f is the frequency, and ϵ r is a relative permittivity. In the design of Vivaldi's taper slot antenna, the dimensions of Tapered length and Tapered rate determines through the calculation using formula (3). The slope level of the taper slot of Vivaldi antenna greatly affects the gain, beam width and bandwidth of the TSA [3].

Tapered slot antennas have a curvilinear level based on exponential functions as in equation (3) where long tapered values was predetermined and the mouth opening value can be found by using formula (4)[4].


Air-coupled on GPR systems is used to evaluate and obtain information from the topside of the infrastructure (such as sidewalks or asphalt roads). Air-coupled antenna system operates on the frequency range 500 to 2500 MHz and the middle frequency is on 1.0 GHz where this frequency has an ability to penetrate ground 0.5 to 0.9 meters [5]. One of the advantages of an air-coupled antenna is that as the process is installed, data processing can be carried out at vehicle speeds of up to 100km/h which does not disturb the traffic around it.

Microstrip to the slot line transition is simply a feed technique by crossing the slot line with the microstrip [3]. This casting technique includes all types of electromagnetic couplings because the slot line and microstrip are separated by substrate elements. Stub is the distance between the midpoint of the microstrip and slot line meeting. Equation (5) is used to determine the wavelength by using a Microstrip pilot for slot line transitions. Table 2 shows Vivaldi antenna dimension parameter values after calculation and Figure 2 shows an initial design of Vivaldi antenna.

Table 1

Parameters of Vivaldi antenna.

Parameters Symbols Value
Tapered Length TL 75 mm
Tapered Rate R 0.0555
Mouth Opening MO 73.22 mm
Stub Length stubL 24.1 mm
Slot line Length sL 74 mm
Slot line Width S 1.14 mm
Antenna Length PA 150 mm
Antenna Width LA 75 mm
Cooper Thickness    - 0.035 mm
Substrate Thickness H 1.6 mm
Backwall offset bwo 1 mm
Microstrip Width W 3.1 mm
Figure 2

Initial design of Vivaldi antenna, front view (a), back view (b).


3. Results

The Vivaldi antenna design with dimension parameters results from the distribution calculation to determine the return loss and VSWR values in the working frequency range as shown in Figure 3.

Figure 3

Simulation result of Vivaldi antenna at first, return loss (a), VSWR (b).


Both graphs show that Vivaldi antenna does not have return loss and VSWR values according to specifications. Therefore optimization is done by changing the parameter values of the dimensions of the antenna width, antenna length and tapered slot. The following Vivaldi antenna parameters after optimization are shown in Table 2 and simulation results with optimized parameters are shown in Figure 4. In Figure 4, return loss value is less than -10 dB and VSWR value is between 1 and 2.

Table 2

Parameters of Vivaldi antenna after optimization.

Parameters Symbols Value
Tapered Length TL 250 mm
Tapered Rate R 0,022
Mouth Opening MO 278, 95 mm
Stub Length stubL 24,1 mm
Slot line Length sL 99 mm
Slot line Width S 1,14 mm
Antenna Length PA 350 mm
Antenna Width LA 300 mm
Cooper Thickness    - 0,035 mm
Substrate Thickness H 1,6 mm
Backwall offset Bwo 1 mm
Microstrip Width W 3 mm
Figure 4

Vivaldi antenna simulation result after optimization, return loss (a) and VSWR (b).


Optimization process

The optimization process is done by changing the antenna length value, antenna width and tapered rate value. For antenna widths, changes are made by making the antenna width larger. Figure 5(a) shows the change in the shape of the return loss graph for some antenna width values which are 75 mm (red), 100 mm (green), 125 mm (blue), 200 mm (orange) and 250 mm (pink). For antenna lengths, changes are made by increasing the antenna width value. Figure 5(b) shows a graph of return loss against several values of the antenna length which are 200 mm (red), 250 mm (green), 300 mm (blue) and 350 mm (orange). For tapered rate values, tapered length values are made even greater, so the tapered rate becomes smaller. Tapered rate simulation is shown in Figure 6.

Figure 5

Return loss, antenna width shifting graph (a) and antenna length shifting graph (b).

Table 3

Tapered length and tapered rate optimization value.

Tapered length (mm) Tapered rate Color
75 0.0555 Red
100 0.04165 Green
150 0.0277 Blue
250 0.022 Orange
300 0.018 Pink
Figure 6

Return loss toward tapered slot value shifting.


4. Discussion

Figure 5(a) shows when the antenna width value is enlarged, the graph gradually moves towards low frequency (return loss and VSWR). This causes greater bandwidth. Next, optimization is performed on the antenna length dimension parameters. Figure 5(b) shows return loss against several values of the antenna length: 200mm (red), 250mm (green), 300mm (blue) and 350mm (orange). When the antenna length is enlarged, there is no significant change in the return loss and VSWR graphs to the working frequency range of the Vivaldi antenna. Antenna length value greater than the antenna width aims to make the Vivaldi antenna still have a radiation pattern which is consistent with its characteristics.

Tapered slot optimization is done by changing two dimensional parameters, which are tapered length and tapered rate. Table 3 shows tapered length and tapered rate optimization values. In Figure 6, it can be seen that when the tapered slot, includes the tapered rate and tapered length values, is increased, the working frequency range of the Vivaldi antenna shifts towards the low frequency (return loss and VSWR). The result when tapered length value is enlarged and tapered rate value is reduced, the working frequency range widens. However, tapered slot optimization is limited by antenna width and antenna length because their dimension depend on the dimensions of the length and width of the Vivaldi antenna.

Figure 7

Fabricated antenna, the antenna (a), return loss measurement (b), VSWR measurement.


Furthermore, the antenna design is fabricated to determine its bandwidth by measuring it using a network analyzer. Figure 7(a) shows the fabricated Vivaldi antenna. The fabricated Vivaldi antenna bandwidth is measured using a network analyzer. Figures 7(b) and 7(c) show the return loss graph and the VSWR of the fabricated Vivaldi antenna. Fabricated Vivaldi antenna shows a decrease in bandwidth and the working frequency whereas the fabricated Vivaldi antenna has a working frequency range from 1 GHz to 1.7 GHz. The bandwidth decrease is caused some error on fabricated antenna that make differences between the dimensions of the Vivaldi antenna simulation and fabricated antenna parameters. Table 4 shows the comparison of the parameters of the Vivaldi antenna dimensions with the fabrication simulation. There are differences in the parameters of the mouth opening dimension, the width of the feed channel and the backwall offset. This causes differences in the results of fabricated and simulated antenna performance.

Table 4

Comparation between optimization and fabrication antenna parameters.

5. Conclusion

The design of the Vivaldi antenna for the Ground Penetration Radar is carried out starting from the literature study, determining antenna specifications, designing and optimizing the shape of Vivaldi antenna on the antenna simulator application and antenna fabrication so that the bandwidth can be measured.

This Vivaldi antenna with dimension 350 × 300 mm has a working frequency range from 1 GHz to 1.7 GHz with return loss values is less than -10dB and VSWR value is between 1 and 2. The fabricated Vivaldi antenna has decreased bandwidth from the simulation results which has bandwidth 1 GHz with a working frequency range from 1 GHz to 2 GHz. However, the fabricated Vivaldi antenna can be used on GPR for Non-Destructive Testing Highway antennas, which the general frequency for Non-Destructive Testing Highway is 700 MHz – 2 GHz.


The authors would like to express their gratitude to the Dean of the Engineering Faculty, Universitas Negeri Jakarta, for the contribution and support to the research.

Conflict of Interest

The authors have no conflict of interest to declare.



H. M. Jol, Ground Penetrating Radar Theory and Applications. Oxford: Elsevier Science, 2008.


P. J. Gibson, “The Vivaldi Aerial,” in 1979 9th European Microwave Conference, 1979, pp. 101–105.


R. Rajaraman, Design Of a Wideband Vivaldi Antenna Array for the Snow Radar. University of Kansas, 1999.


Y. Erdogan, Parametric Study and Design of Vivaldi Antennas and Arrays. Ankara, Turki: Middle East Technical University, 2009.


T. Hariyadi and M. Mukhidin, “Studi Parametrik Antena Vivaldi Slot dengan Pencatuan Mikrostrip,” in Seminar Nasional Teknologi (SENATEK) 2015, 2015, pp. 397–403.



  • Downloads 2
  • Views 11



ISSN: 2518-668X