Passive RFID Tag for Railway Application

Passive RFID tags based on narrow band absorbers are proposed for railway applications. The tags consist of absorbing tiles of size 30 × 30 cm. The designs of these narrow band absorbers are presented based on infinite array approximation by using periodic boundary conditions. Then, the radar cross sections (RCS) of finite tiles of these designed absorbers are compared with the corresponding RCS of a conduction plate of the same size of the tiles. The difference between the RCS of the absorbing tiles and the conducting tiles corresponds to the RFID digit “1” or “0”. An experiential verification for a sample of these narrow band absorbers is presented based on measuring a finite tile inside a transverse electromagnetic (TEM) cell. The design of this TEM cell is also discussed in detail.


Introduction
Radio Frequency Identification (RFID) is a technique that combines radio frequency with computer system to introduce a wireless automatic identification system [1]. RFID systems are being applied to many applications. Generally, RFID system consists of a reader, an RF module, an antenna and a tag [1]. RFID tag can be classified into two main categories: active and passive namely. The main difference between passive and active tags is that active RFID tag is powered through an internal power source; whereas passive RFID tag responses to the incident RF energy transferred from the reader to the tag when the tag is passing through the reader [1] [2].
Identification process for railway application has a significant importance in many cases like determining the location and the speed of the railway vehicles. Railway vehicle identification system consists of information collection, processing and transmission subsystems as shown in Figure 1. RFID system is a key component of the railway vehicle identification system. In Railway Vehicle Identification system, each vehicle is equipped with a unique tag which is mounted on the vehicle. This tag contains the identification data of this vehicle.
The tag has its response when it passes by the reader. The readers are usually located at fixed points separated by equal distances. The RF reader is designed to collect the vehicle identity sent from the Tags. The Reader is connected to a computer control system. Once the Reader receives the vehicle identity from the Tag, the Reader reports the associated vehicle arrival or departure information at this location to the control system. The control system then captures this data for further processing [3]- [9]. General RFID tracking system for vehicles and their main applications are discussed in [10]. These systems include traffic signal timings, congestions on the road and theft of vehicles. The difference in the case of railway application is that the train travels on a specified constant way while other vehicles have different directions and locations. This property of railway vehicles simplifies the implementation of RFID in this application. Different examples of RFID systems for railway application are discussed in [3]- [9]. Different problems are also discussed in these cases like high speed train, data collision and insufficient reading time. An example for this RFID system is active RFID tag which uses an inductive coil with the tag and a permanent magnet on the railway to activate the tag while the train is moving with respect to the fixed magnet. However, the operation of this system depends on the speed of the train at the reading point. Thus, the validity of this system may not be assured for all speeds. On the other hand, a fully passive printable chipless RFID system based on multi-resonators is presented in [10] [11] [12]. This chipless tag uses the amplitude and phase of the spectral signature of a multi-resonator circuit. The amplitude and phase of the backscattered field from this tag provide the corresponding data bits. In this case, the tag consists of microstrip multi-resonators and cross-polarized UWB (Ultra Wide Band) transmitting and receiving antennas. In this case, the used UWB is the unlicensed FCC UWB in the frequency range from 3.1 to 10.6 GHz.
However, this tag is usually very small for large targets like trains. Also, it may not be suitable for high speed vehicle since the available reading time is very short. In this paper, we present a new idea for a passive tag which is suitable for large targets. The idea of the proposed tag is based on attaching narrow band absorbing tiles on the side wall of the train. These absorbing tiles play the same role of the multiple resonators but with larger size which is suitable for the railway application.
This paper is organized as follows. Section 2 presents the basic design of narrow band absorbers which are used as the elements of the proposed passive RFID tag. These narrowband absorbers are composed of periodic patches on a grounded lossy dielectric slab. These periodic structures are designed by simulating a single element in periodic boundary conditions. The designed elements are used to simulate finite size tiles which are used as absorbing tiles on the train.
The radar cross section (RCS) of these finite tiles is compared with the corresponding RCS of PEC tiles of the same size. The difference between these two RCS values represents the obtained data by the reader. In Section 3, an experimental verification of a sample of these narrow band absorbers is presented by using TEM cell. Finally, Section 4 presents the conclusion.

Unit Cell of Narrow Band Absorber
The proposed RFID tag is composed of multiple narrow band absorbers. These absorbers are based on periodic patches on a lossy grounded dielectric slab [13] [14] [15]. These patches are also covered with a superstrate. This superstrate is   In this case, each absorbing frequency can be used as a different digit in RFID system as in the case of multi-resonator RFID tag [10] [11]. It can be noted the reflection coefficients of the proposed absorbers at the absorbing frequencies for the case of square patches are around −20 dB in most cases. These values can be improved to be less than −25 db in Hexagonal patches and to be less than −30 dB in circular patches in some cases. Thus, it can be concluded that different shapes are suitable for different frequencies. As an example, square patches are suitable for frequency 3.56 and 3.89 GHz, hexagonal patches are suitable for frequencies 2.93 and 3.33 GHz and the circular patches are more suitable for the frequencies 4.37 and 3.58 GHz as shown in Figure 3.

RCS of Finite Absorber Tiles
In practical case, finite absorber tiles are used. Thus, the previous simulation of Open Journal of Antennas and Propagation S. A. El-Rahman et al.
infinite array structure by simulating a single element in periodic boundary conditions can only be used as a starting point for the design of finite absorber tile [16]. The proposed tiles have dimensions 30 × 30 cm 2 as shown in Figure 4 for different patch configurations. In the proposed application, the corresponding digit of each tile is "1" or "0" based on the presence of the absorber tile or not.
This difference can be detected by comparing the RCS of the tile to the corresponding RCS of a PEC tile of the same size. This is mainly the function of the reader which should be fixed at a constant distance from the railway. Figure 5 shows the RCS of samples of these finite absorbers at their corresponding resonance absorbing frequencies compared to the RCS of PEC plate of the same size at these frequencies. It can be noted that difference between the RCS of the finite absorber tile and the RCS of the PEC is about 12 dB for square patches, 8 dB for hexagonal patches and 14 dB for circular patches. It can be noted that these finite absorber tiles can be designed to introduce RCS differences more that 10 dB compared with PEC tiles for most cases. This 10 dB is quite enough to discriminate between the absorber tile and the PEC tile. Thus, it can be used as an RFID digit. In the following section, an experimental verification for the circular-patch absorber is presented as an example for these finite tiles.

Experimental Verification of Narrow Band Absorber Tile
In this section an example of the above designed absorber tiles is verified experimentally. To synthesize an equivalent incident plane wave, we used a TEM cell [16] [17]. The TEM cell consists of two tapered transmission line sections connected to a parallel plate waveguide as shown in Figure 6. The height of the parallel plate waveguide is chosen to be the same as the periodic cell of the absorber tile which is 3 cm.
This parallel plate waveguide can be used to represent equivalent periodic structure in the perpendicular direction to the parallel plates by applying the image theory. However, the structure along the width of the parallel plate waveguide would be finite. The dimensions of the proposed TEM cell are designed and optimized numerically by using HFSS. The final dimensions of the TEM cell are as shown in Figure 6. Figure 7 shows the simulated electric field distribution along the designed TEM cell at 4.35 GHz. It can be noted that the field distribution at the center of the parallel plate waveguide is nearly uniform plane wave. This layer was also included in the simulation. A slight slit is presented in the foam layer as shown in Figure 8. This slit is used to insert or remove the absorbing sheet as shown in the following results. Figure 9 shows a comparison between the simulated and measured reflection coefficient of the TEM cell without any sample inside it. Figure 10 shows the simulated comparison between the S 11 for the TEM cell with and without the absorbing tile. In this case the absorbing tile is based on circular patches with radii R = 10 mm which satisfy absorption at 4.35 GHz as discussed in Figure 3(c). The tile in this case is composed of only four patches as shown in Figure 11. These four patches are equivalent to infinite array in the z-direction inside the TEM cell by applying the image theory. It can be noted from Figure 10 that the simulation results show a significant reduction more than 20 dB in the measured reflection coefficient at the designed absorption frequency.
This result is quite consistent with the simulation result of the corresponding infinite array structure in Figure 3(c). Figure 12 shows the comparison of the measured results of S 11 with and without the absorbing tile. Excellent agreements between measured results shown in Figure 12 and simulated results shown in       patches. The design procedure starts with simulation of an infinite array structure by using a single element inside periodic boundary conditions. Then the RCS of a finite tile of the designed array of patches is compared to the RCS of a PEC tile. The difference between these two values of the RCS corresponds to the difference between the digit "1" and "0" at the corresponding absorption frequency. Each shape shows a good behavior at specific frequencies. An experimental verification for the design of these absorbers is present for the case of circular patches by using TEM cell. The design of this TEM cell is also discussed in detail. Excellent agreements between simulated and experimental and simulated results are obtained.