Design parameters.
Abstract
Wireless LAN usage is also increasing at construction and civil engineering sites, and the efficiency of ICT construction has increased due to the use of tablet PCs and network cameras. When constructing a wireless LAN environment, for example, a LAN cable may be laid from outside the tunnel, and a number of wireless access points (APs) may be installed. However, it is not advantageous to use a large number of APs because the system price increases significantly. We consider using a long leaky-wave antenna to provide one AP. The reason for using a leaky-wave antenna is that, since the total tunnel length is on the order of km, it is necessary to reduce the power radiated by the antenna as much as possible to provide a functional communication area over a long distance. To reduce such transmission losses, we used a waveguide. A waveguide is a low-loss line and can function as a low-loss and low-radiation leaky-wave antenna which is suitable for long-distance communications; this is accomplished by combining a waveguide with a low-radiation antenna mechanism. In this chapter, we report the development of a waveguide-type leaky-wave antenna and the development of a wireless LAN environment in a tunnel.
Keywords
- wireless communication
- microwave
- waveguide antenna
- long distance
- low radiation
1. Introduction
In recent years, wireless LANs have become widespread and are indispensable for convenient Internet use. Wireless LAN usage is also increasing at construction and civil engineering sites, and the efficiency of ICT construction has increased due to the use of tablet PCs and network cameras. Remote monitoring of worksite interiors contributes greatly to more rapid construction. This means that construction of wireless environments in the field is indispensable. Tunnel construction often takes place in the mountains. An LTE (4G) line may become disconnected but it cannot connect at all to the line in the tunnel.
This is because it is difficult to transmit radio waves from outside the tunnel to the inside. Radio waves are reflected and absorbed by thick soil and concrete walls, and this means that no external radio waves can be received inside the tunnel [1]. Therefore, it is common to lay a wired line from the outside of the tunnel and to construct a telephone line or other types of communication line in the tunnel. When constructing a wireless LAN environment, for example, a LAN cable may be laid from outside the tunnel and a number of wireless access points (APs) may be installed. However, working with a wired line is complicated, and there is a high risk of disconnection due to contact with building materials and construction equipment. Therefore, a high degree of robustness with fewer system failures is also required. Also, it is not advantageous to use a large number of APs because the system price increases significantly.
Therefore, we consider using a long leaky-wave antenna to provide one AP. The reason for using a leaky-wave antenna is that, since the total tunnel length is on the order of km, it is necessary to reduce the power radiated by the antenna as much as possible to provide a functional communication area over a long distance. The use of leaky coaxial cable (LCX) as a leaky-wave antenna has been studied [2, 3, 4, 5, 6]. As shown in Figure 1, a long-range communication area can be constructed by reradiating the output of the AP from a long LCX. However, in practice, the available power is attenuated in the cable due to transmission losses (mainly dielectric losses) of the LCX, so it is difficult to communicate over long distances.
To reduce such transmission losses, we used a waveguide [7]. A waveguide is a low-loss line and can function as a low-loss and low-radiation leaky-wave antenna which is suitable for long-distance communications; this is accomplished by combining a waveguide with a low-radiation antenna mechanism. In this paper, we report the development of a waveguide-type leaky-wave antenna and the development of a wireless LAN environment in a tunnel. We evaluated the system in the W56 band (5.5–5.7 GHz), as specified by IEEE 802.11 “a”, “n” and shown in Figure 2.
2. Overview of the waveguide antenna
A waveguide is a hollow metal tube and transmits radio waves using reflections within the tube. In particular, rectangular waveguides are used in various applications such as radar, microwave oven, and microwave feeds. Transmission losses are low even in a microwave band or in a millimeter-wave band, and waveguides are expected to be used as transmission lines for next-generation communications.
A waveguide has a rectangular cross section as shown in Figure 3, and radio waves are transmitted by reflecting between the two metal plates on both ends of the waveguide at an angle
Since the reflected waves at both ends are combined into one wave in the waveguide, the wave is transmitted within the waveguide at the guide wavelength
This paper deals with the TE10 mode, which is the most basic transmission mode. In this mode, the current and electric field shown in Figure 5 flow through the waveguide. For this case, if a slot is provided that is orthogonal to the current direction, radiation is emitted from the slot, and a waveguide antenna is created.
A traveling-wave antenna is one that continuously emits energy by using a traveling wave; surface-wave antennas using a dielectric line and leaky-wave antennas using a waveguide or coaxial line are well known. As described above, a leaky coaxial cable (LCX) is utilized as a highly flexible traveling-wave antenna by creating a slot in the outer conductor. However, LCX is not suitable for long-distance applications due to its large dielectric losses in the 5 GHz band.
In the future, as the frequencies used shift to quasi-millimeter-wave or millimeter-wave communications, dielectric losses will increase. A waveguide is considered to be useful because it has no dielectric losses and has small overall transmission losses. Figure 6 shows a general traveling-wave leaky waveguide (with a phase constant
When a continuous slit is present, the amount of radiation power increases, and the remaining power in the waveguide decreases. To apply this method to the proposed tunnel system, it is necessary to not only reduce the transmission losses but to also reduce the radiation levels and to maintain power in the pipe over long distances.
3. Dual-plate leaky waveguide
The traveling-wave type of leaky waveguide shown in Figure 6 requires a slit that is continuous in the direction of tube length, and such fabrication may increase the cost. To obtain a waveguide that is significantly cheaper than LCX, we need to minimize the number of processing steps for the tube. Therefore, we consider creating a waveguide (Figure 7) with a slit mechanism that is constructed by combining two U-shaped plates (metal plates). Bending such metal plates does not require a mold and they are easy to manufacture [10].
In the present waveguide, a slight gap is created between the plates, and the thickness is adjusted by sandwiching a thin insulating sheet or similar material. When viewed in the cross-sectional view, the present waveguide has the structure shown in Figure 8(a), which is equivalent to the structure shown in Figure 8(b). As shown in Figure 9, the results from the analysis of the transmission characteristics, as shown in Figure 8(a) and (b), are nearly the same.
Radiation is generated by the magnetic field which is generated in the opening of the waveguide. This is because the current flowing in the slit is determined by the
When the impedance at the slit as viewed from inside the waveguide is low and when the slit height
40 | 20 | 0.05 | 0.05 | 20 | [mm] |
The far-field radiation wave pattern and gain at 5.7 GHz of the designed waveguide were analyzed by simulation (Ansys HFSS). Figures 10–12 show the results.
The radiation directly above (on the
The waveguide must retain sufficient residual power over long distances. First, the conduction losses were examined. The conduction losses depend on the conductivity of the metal used for the waveguide, as shown in Figure 14. The waveguide discussed herein is made of aluminum, which has relatively good electrical conductivity; aluminum was used to manufacture the waveguide at a low cost. In addition, it is necessary to suppress the radiated power and reduce leakage. Therefore, whether the leakage can be reduced by adjusting the design parameters was examined. Here, it is assumed that there were no conductor losses.
First, the radiation loss when the slit height
In addition, the radiation increases due to the lower attitude. This is because the current increases. Although the degree of freedom and convenience of installation are improved by decreasing the waveguide profile, it has been confirmed that there is a trade-off. Naturally, when the profile is lower, the conductor losses for the waveguide increase. In this study, we focused on the radiation characteristics, but we also need to consider conductor losses.
Next, the radiation losses when the slit width
Since the characteristic impedance at the slit varies with Δ
Finally, Figure 17 shows the radiation losses when the slit length
However,
4. Evaluation of the communication experiment
The leaky waveguides were cascaded using joints. In this study, a non-leaky waveguide was used for the joints and the design was modified as shown in Figure 18. The insertion length of the leaky waveguide was 14 mm (≒
Figure 20 shows the configuration of the experiment. The access point (e.g., ACERA 850F, FURUNO) was connected to the leaky waveguide via a coaxial waveguide conversion connector, and the leaky wave from the waveguide was received by the receiving antenna. At this point, the orientation of the receiving antenna from the waveguide was set as the
As a result of laying the waveguide over 120 m and measuring the power with the spectrum analyzer located at the end, it was found that the loss was 35.8 dB, i.e., approximately 0.32 dB/m. The output frequency was 5.6 GHz and the bandwidth was 40 MHz. Figure 21 shows the evaluated throughputs and S/N ratios for the conditions
5. Conclusion
In this research, we proposed a low-leakage dual-plate waveguide and demonstrated the results of evaluating long-distance communications using this waveguide. As a result of this evaluation, under the conditions of
Acknowledgments
I am grateful to Dr. Patrick Steglich of the book editor who gave me the opportunity to write this chapter. We thank Mr. Nobuyuki Watanabe and Mr. Toshifumi Sakai (FURUNO) for their help in this study. Moreover, I respect the great achievements of my predecessors whose studies I have cited.
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