A novel multi-band end-fire antenna array was designed, fabricated, and characterized. Analytical calculations were carried out to determine the critical antenna dimensions and the design was optimized using a 3D electromagnetic finite-element solver. The measured results were in good agreement with the designed results. The proposed antenna array exhibits multi-band capabilities which can be potentially used for applications that require a multi-band end-fire radiation pattern.
Traditional base stations employ omnidirectional antennas where the transmit power is equally radiated in all directions. The equal distribution leads to a portion of the power being transmitted throughout the cell but not received by the user. This wasted power then becomes forward link interference to other base stations or users in other cells. Similarly, each new user added to a cell increases the interference and noise levels on the reverse link. This results in a reduction in the signal-to-noise ratio, which in turn degrades the performance of the detection and demodulation operations. One way to address this problem is in the design of the antenna having multiband end-fire properties with sectorized radiation patterns (wide beamwidths) and high gain (above 5 dBi) in order to create a high front-to-load ratio and alleviate propagation loss effects.
In order to respond to the above need, a novel end-fire antenna array has been investigated using microstrip antenna theory. The microstrip patch antenna was first introduced by Munson in a symposium paper in 1972 [
The rectangular patch end-fire array antenna consists of a half-wavelength by 0.12-wavelength microstrip elements printed on the top substrate layer and connected to a quarter wavelength microstrip corporate feed-line. The ground plane is printed on the bottom substrate. This avoids using a half-wavelength balun, thereby simplifying the antenna geometry. The multi-band behavior is obtained when TM modes can be excited simultaneously. By properly selecting the location of the corporate feed line and optimizing the element width, the antenna can resonant at multiple frequencies [
In this paper we present the theoretical description and design methods used in modeling the rectangular patch end-fire array antenna. Comparison with the fabricated end-fire patch antenna array is described.
End-fire operation is established when the direction of the radiation for the main beam is dependent on the phase difference, α, between the elements of the array. Therefore, it is possible to steer the main beam in any direction by varying α between elements. We start with considering a linear array antenna consisting of N elements, equally interspaced a distance d. The direction of a wave is described by the angle θ between rays and array normal. Therefore, the array factor, AF(θ), for a receiver linear array antenna is given by
where is the wave number and λ is the wavelength [
thus,
The normalized array factor is given by
So for ψ = 0, an end-fire operation at θ0 = 90˚ and θ = −90˚, respectively, the phase difference, α, between two adjacent elements is [8,9]
and
High front-to-back ratio is required for an efficient endfire operation. This is achieved by reducing the occurrence of grating lobes to below zero. According to antenna theory, grating lobes occur whenever the argument ψ is an integer multiple of 2π. Therefore, at end-fire operation, grating lobes occur for
For a multi-band linear array antenna we could space the elements as far apart as one wavelength before seeing any grating lobe effects. However, for a linear end-fire array antenna the maximum allowable element spacing is reduced to half a wavelength to prevent the occurrence of grating lobes. If we reduce the element spacing even farther, by less than half a wavelength, the grating lobe at θ = −90˚ becomes less visible.
The main advantage of the rectangular patch end-fire array antenna lies in its simplicity of design. This allows for a model-based analysis in a short amount of time and, given some user-defined parameters, the design can be optimized. This antenna was designed and simulated using Ansoft HFSS, a 3-D electromagnetic simulator [
The antenna consists of eight radiating elements connected to a full corporate feed configuration encompassing both branch and main feed. Figures 1(a) and (b) show dimensions and a photo of the proposed fabricated multi-band end-fire array antenna at its optimum RF board configuration, respectively. The resonant frequency for its transverse magnetic (TMmn) mode can be evaluated from [
where c is the velocity of light; m and n are integers; L and W are the length and width of the patch element, respectively; and εr is the relative permittivity of the substrate. The width of the patch element can be described as [11-13].
The four lower order modes, namely TM01, TM20, TM30, and TM40, have been predicted by Equation (8) and the resonant frequencies of the proposed antenna changes slightly with the alteration of the width, W, hence, after obtaining rough estimate from Equation (9), HFSS optimization was performed. The optimization process is shown in
Based on the above discussion on antenna width and length, a length of 0.5λ and a width of 0.12λ for the rectangular patch element were chosen.
The element distance, d, that would ensure end-fire operation along the x-y plane was then found. Using Equation (11), where D is the antenna directivity, d in range of 0.04λ to 0.05λ was found and then optimized with HFSS [
The rest of the dimensions (A, B, C, E and F) were determined using HFSS optimization routine.
To verify the analysis presented for this antenna structure, the antenna was measured. The design was fabricated by Advanced Circuits, and measured in the microwave laboratory of the Engineering and Applied Science (EAS) building at the University of Colorado at Colorado Springs. The antenna was fabricated in FR-4 substrate with a dielectric constant of 4.25 and a thickness of 62 mils. The radiation pattern was measured in the anechoic chamber of the EAS building. The antenna was mounted on a polystyrene foam platform with a standard clear tape and connected to a coaxial cable. The antenna-under-test (AUT) served as the receiving antenna, while a rectangular horn antenna was used to transmit the wave. Due to the design of the platform, only an E-plane measurement in the range of −178˚ ≤ θ ≤ 178˚ could be taken. This was sufficient to compare the main beam and the backside radiation level.
the multi-band end-fire antenna array. The proposed antenna produces an end-fire beam and is matched over a multi-band in the frequency range of 2.0 to 4.5 GHz. Multi-dips in S11 were measured, which includes impedance matching at frequencies of 2.9, 3.4, 3.7 and 3.9 GHz.
The design, fabrication and characterization of a rectangular patch end-fire array antenna were presented. The antenna was designed and optimized using eight elements of half-wavelength and a width 0.12λ in FR-4 substrate. Measured results showed end-fire operation with a measured maximum gain of 6.9 dBi in the end-fire direction. The proposed antenna can be employed for multiband applications that require a radiation pattern in the end-fire direction.
Although the research achieved its objectives, the antenna has an inherent limitation in its pure form. Namely, if the end-fire array is confined to operate in receiving mode, detuning may occur should changes in climatic or atmospheric conditions develop. Additional testing, such as the Over-the-Air (OTA) testing, could be conducted in order to accurately measure the antenna’s performance in environmental conditions. Furthermore, in the radiation pattern measurement, the operating frequency was limited to operate at a single frequency. By measuring additional radiation patterns at each of the frequencies shown in