Advances in LowProfile Antennas in Wireless Communications 2015
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Substrate Integrated Waveguide LeakyWave Antenna Conforming to Conical Shape Surface
Abstract
A conical conformal leakywave antenna based on substrate integrated waveguide (SIW) technology is proposed and demonstrated in this paper. This antenna conforms to a conical shape surface with the angle of 40°. It has a narrow beam that scans from 80° to 97° with varying frequency (34 GHz~37 GHz). Both conformal and nonconformal antennas are fabricated through the standard PCB process. Their performances are compared within the desired frequency.
1. Introduction
Conformal antennas have been of wide interest to scholars due to the purpose of integrating with the structures such as part of airplane, train, or other vehicles. The theory and design of conformal antennas are fully described in [1]. Different surfaces can be used in conformal antennas, such as a cylindrical shape, a conical shape, and a spherical shape. Among them, the conical shape surface can be of special interest for applications in the noses of missile, aircraft, and instrument.
As is well known, leakywave antennas are a member of the family of travelingwave antennas that permit the power leaking along one of their sides, and the radiation patterns can be scanned by varying frequency [2]. Many researchers have studied numerous types of leakywave antennas. The leakywave antenna in [3] generates leakage when the period length between the vias is sufficiently large. A leakywave antenna based on the halfmode substrate integrated waveguide (HMSIW) discussed in [4] possesses the qualities of compact size, wide bandwidth, and quasiomnidirectional radiation pattern. The long slot leakywave antenna [5] has the controllable side lobe level by changing the position of vias in its sidewall. A microstrip leakywave antenna (MLWA) performance on a curved surface [6] provides an alternative to the traditional resonant microstrip antennas. A fixedfrequency beamscanning MLWA array [7] has the capability of scanning the main lobe continuously at the fixed frequency by controlling the relative phase between two elements. An HMSIW leakywave antenna with a series of ±45° slots published in [8] can provide four states of polarization (linear or circular) according to the different input ports. A novel leakywave antenna with transverse slots is proposed in [9] that has the advantage of scanning to endfire. It radiates from a periodic set of transverse slots on the top of the substrate. The leakywave antenna designed on a composite right/lefthanded (CRLH) SIW [10] has beam scanning from the backward to the forward direction and operates in two frequency bands. A low temperature cofired ceramic (LTCC) leakywave antenna based on the substrate integrated image guide (SIIG) is realized in [11], and it has both the simplicity in designing procedures and better fabrication reliability.
The conformal leakywave antenna has a simple structure, high efficiency, and ability of frequency scanning. Therefore, some useful conformal leakywave antennas have been introduced. The cylindrical microstrip leakywave antennas implemented in [12] have the high gain and wide bandwidth, similar to those of the planar ones. A novel theory to analyze and design tapered conformal leakywave antennas [13] shows how it can maintain the desired highdirective scanning performance in spite of the curved shape. By comparing among the nontapered rectilinear antenna, nontapered conformal antenna, and the tapered conformal antenna [14], it presents how the antenna width needs to be tapered along the antenna length to properly synthesize the complex propagation constant and therefore to produce a desired radiation pattern.
As a new guidedwave structure, substrate integrated waveguide (SIW) has attractive advantages including low loss, low cost, easy fabrication, and convenient integration with planar circuit [15–17]. Meanwhile, SIW has the good conformability and fullclosed topology to avoid the unwanted leakage, which is a great impetus for the deployment of millimeterwave integrated conformal array antennas [18]. In this work, a SIW leakywave antenna conforming to a conical shape surface with the angle of 40° is introduced. It is fed by the standard WR28 waveguide. The antenna is designed and simulated using the fullwave simulation software Ansoft HFSS. parameter and radiation patterns are also investigated. The experimental results agree well with simulations.
2. Conformal SIW LeakyWave Antenna Design
The prototype SIW leakywave antenna is shown in Figure 1(a). The antenna leaks power through the SIW side wall by changing the window gap [3]. This antenna is embedded in a conical base as shown in Figure 1(b). The conformal cone has the angle of ; the conformal beam direction is in the xoy plane (about theta = 90°). To realize this, the leakywave antenna should has the beam direction of (the angle between the axis and the beam direction in Figure 1(a)). Here, the antenna radiates at the backward direction.
(a)
(b)
Firstly, the leakywave antenna will be designed. The substrate used here is the Rogers 5880 substrate with the thickness of 1.575 mm, the relative permittivity of 2.2, and the loss tangent of 0.0009. The main parameters of the leakywave antenna are the SIW width, , the distance between the leakywave part and the edge of the substrate, , the length of the leakywave part, , and the leakywave window gap, , where is the number of windows. The designed frequency is at 35 GHz.
The complex propagation constant of the leakywave antenna iswhere is the leakage rate and is the leakymode phase constant. The beam direction of the leakywave antenna mainly depends on [2]. Consider In (2), . The desired beam direction can be realized when changing appropriately. The radiation efficiency due to the absorbed load directly depends on the normalized leakage rate and the leakywave part length A typical choice for the radiation efficiency is 90%.
For the proposed antenna, and can be easily controlled by changing the parameters and . Figures 2, 3, 4, and 5 show the performances of and when and are varied. In order to avoid the appearance of undesired channel modes, is usually set to less than [2]. The length mainly influences the radiation efficiency due to the absorbed load. The relationship between and radiation efficiency is listed in Table 1.

To synthesize the desired radiation properties, we finally choose the parameters of leakywave antenna as follows: mm, mm, mm, and mm (). The beam direction of single antenna is 130°. As shown in Figure 6, of such a twoport antenna is below −13 dB within 34~37 GHz. Considering 95% energy leaking along SIW, only one port architecture is used in the later simulation and fabrication.
The designed oneport leakywave antenna is conformed to the cone. A long groove is cut on the surface of cone, and the antenna is inserted into the groove. The parameter and radiation patterns of the conformal and nonconformal antennas are compared in Figures 7, 8, and 9. As shown in Figure 7, their are almost below −10 dB within 34~37 GHz. The conformal gain (15.5 dBi) is higher than the nonconformal one (15.2 dBi) because of the secondary reflection after conforming to the cone. Moreover, the conformal beam is wider than the nonconformal one in the azimuth plane.
Figure 10 shows the conformal beam scanned from 80° to 97° by varying frequency in the elevation plane. When the frequency is increased, the beam moves to a small theta angle. In the azimuth plane, the beamwidth is mostly affected by the conformal geometry. As shown in Figure 11, by decreasing the curvature of conformal cone from 13 m^{−1} to 10.5 m^{−1}, the 3 dB beamwidth is narrowed from 34.6° to 31.3°. Meanwhile, the gain increases by 0.5 dB.
3. Measurement Results
A prototype antenna is fabricated to validate our design as shown in Figure 12. The antenna is excited by the standard WR28 waveguide; the transition between standard waveguide and SIW has the similar configuration as described in [19]. A coupled aperture is etched on the top conductor layer as shown in Figure 12(a). The purpose of the designed corner in Figure 12(a) is to make the excitation vertical to the horizontal plane. The reflection coefficients of the conformal and nonconformal antennas are measured by the network analyzer. As shown in Figure 13, the measured parameters are almost below −10 dB within 34~37 GHz.
(a)
(b)
The radiation patterns of conformal and nonconformal antennas are measured in a microwave anechoic chamber. As shown in Figures 1415, the measured results have the same trend of the simulated ones.
Then, the radiation patterns of conformal antenna are measured at different frequencies from 34 GHz to 37 GHz as shown in Figure 16. Table 2 summarizes the measured data. In the azimuth plane, it can cover an angular region of 40.9°. The radiation patterns with different conformal curvatures are also measured as the simulation as shown in Figure 17. The 3 dB beamwidth is narrowed with 3.2°.

4. Conclusion
A conical conformal leakywave antenna based on the SIW technology is designed and experimented. It presents a wide beamwidth in the azimuth plane and a narrow beamwidth in the elevation plane. This conformal antenna can scan from 80° to 97° with varying frequency (34 GHz~37 GHz). The measured antenna characteristics agree well with the simulations. Besides, the antenna has the advantages of low loss, high efficiency, and simple configuration.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgments
This work is supported in part by Program for New Century Excellent Talents in University under Grant NCET130089 and by the State Key Laboratory of Millimeter Waves under Grant K201315.
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Copyright
Copyright © 2015 W. N. Huang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.