# Directive Microstrip Antennas for Specific Below −2.45 GHz Applications

Authors: E. Ávila-Navarro; C. Reig
Journal: International Journal of Antennas and Propagation
 (2012)

---

## Abstract

Microstrip printed antennas are the preferred choice in high data ratio modern communications, mainly at 2.45 GHz and above. In this paper, we propose two different approaches of microstrip printed antennas for lower frequency usage. In this sense, we present a printed microstrip Yagi-like antenna at 868 MHz and a printed dipole log-periodic antenna for wider band applications. We focus on the use of low-cost substrates, with a good performance at these frequencies, and giving antennas with useful sizes for such applications. For the analysis, we make use of standard experimental characterization combined with full-wave 3D-FDTD specifically developed simulations. In this way, the S11, radiation patterns, and gain/efficiency figures are given.


---

## Body

## 1. Introduction

Nowadays, printed antennas are widely used for common mobile communication applications. Every cellular gadget includes one or more integrated antenna in order to match the specifications of the different communication protocols, the most of them under the 802.11x umbrella. In fact, typical GSM and related communication channels are progressively moving to higher frequency layers. Driven by these technological requirements, research on compact antennas is mainly focusing on small omnidirectional antennas for 2.45 GHz, and above [1].Nevertheless, even though printed technology is not restricted to high frequency communications, only few efforts have been carried out in order to scale successful antennas to lower frequency applications, mainly ISM (International Scientific and Medical) ranges [2]. In this sense, RFID applications appear as good example of low-frequency printed antennas. This is a particular case, because the antennas are normally designed as radiating coils due to the low range of utilization [3].For long range and low-frequency applications, wired antennas (Yagi-Uda and related designs) are commonly recommended. They are cheap, robust, easy to install, and their integration with the associated electronics, within a radome, is usually, a straightforward task. Only the absolute size, in some cases, can be considered a handicap [4].We propose to exploit the knowledge achieved with the design of 2.45 GHz antennas in order to translate them to applications below this frequency. At frequencies below 2.45 GHz, the losses tangent of low-cost substrates allows their use with more than acceptable efficiency figures [2]. In this sense, emerging technologies like direct material printing open new possibilities in this field, leading to compact, cheap, and flexible designs, useful for this kind of applications [5]. In addition, novel designs can reduce the overall size of the antenna in order to make it useful for standard applications [6].In order to demonstrate these asserts, in this paper, we describe several microstrip printed antennas for different below −2.45 GHz applications, making use of previous successful designs. For demonstrating our proposal, we describe in detail two different designs, for narrow band and for wider band applications. We firstly present a Yagi-like antenna that can be used in wireless sensor network deployments or even for terrestrial digital television broadcasting links. Then, we also describe a log-periodic printed antenna for wider band applications or parabolic antenna feeding. With all these designs we will demonstrate the potentiality of low-cost substrate printed antennas within these scenarios.The more important parameters of the antenna were simulated and measured. For the calculated results an in-house 3D-FDTD algorithm was used. The code was initially designed for radar antennas analysis [7] and then was adapted for electrical parameters calculations [8] and microstrip printed antenna modelling [9]. The measures were carried out with a vectorial network analyser within an anechoic chamber.


## 2. Results

The presented antennas are fabricated by making use of a standard low-cost FR4 substrate, typically used in printed circuits designs, with a widthh=1.52mm and relative dielectric constant of 3.9 at the used frequency range.


### 2.1. Yagi-Like Antenna

This antenna is proposed for open field wireless sensor networks applications at the free license 868 MHz band. In a particular application [10], some weather stations are located in different and remote places in a wide region (10 × 10 km2). For far end-node stations, standard directive Yagi-Uda antennas are normally used. Printed antennas are proposed as a good alternative for this kind of applications, because their low price and the possibility of integration with the nonmetallic box of the electric sensing devices.The scheme of the Yagi-like antenna is shown in Figure1. The antenna consists on a dipole with the arms located in both sides of the dielectric substrate and a number of director elements with the same dimensions. The dipole is fed by a strip line printed on both sides of the substrate. This scheme of the driver provides the necessary electrical phase to each arm of the dipole, without external elements, allowing a reduction of the final size of the antenna. At the bottom side of the dielectric substrate a truncated ground plane is located. This ground plane acts as reflector element of the antenna [11].Figure 1
Yagi-like antenna scheme.The dipole length is slightly smaller thanλ/2 at the work frequency and the other dimensions of the antenna are obtained by parametric simulations with our 3D-FDTD algorithm [12].The Yagi-like printed antenna is designed for an 868 MHz frequency work onto a piece of low-cost FR4 substrate. Due to final size of the Yagi-like antenna at this low frequency, only two director elements are considered. The optimized dimensions of the antenna are summarized in Table1. In Figure 2 we show the fabricated prototype of the Yagi-like antenna.Table 1
Yagi-like antenna dimensions for 868 MHz.
LDIP = 124.1 mmDDIP = 69.1 mmLDIR = 101.5 mmDDIR = 69.1 mmw = 3.2 mmLM = 180 mmWM = 42.3 mmFigure 2
Fabricated prototype of the 868 MHz Yagi-like antenna (ruler in cm).The measured and calculated return losses are presented in Figure3. A good agreement between both results is obtained, with a measured bandwidth of 138 MHz, around 15% of the central frequency.Figure 3
Simulated and measured return losses of the 868 MHz Yagi-like antenna.The measured and calculated normalized radiation patterns of the Yagi-like antenna for the principal planes at 868 MHz are presented in Figure4. As observed, the antenna displays a directive behaviour with a measured gain of 7 dBi. The estimated antenna efficiency was around 92%.Simulated and measured radiation patterns of the 868 MHz Yagi-like antenna.
(a)
E plane(b)
H planeIn Figure5 we show the normalized electric field distribution Ey component in the middle point of the dielectric substrate at 868 MHz. It is well appreciated that the antenna is fed with the correct phase at the operation frequency.Figure 5
Field distribution of the 868 MHz Yagi-like antenna.


### 2.2. Log-Periodic Antenna

In this paragraph we focus on a wider band design. The range of application of such antennas is well stated [13]. Our particular design includes the L-band and the standard Wi-Fi band, as an example of integrating both technologies.The antenna scheme is shown in Figure6. The antenna consists of a number of printed dipoles with the arms printed in both sides of the dielectric substrate alternatively. Shorter dipoles are located close to the feed point. A strip line printed on both sides of the substrate is used to feed all dipoles. This scheme provides the necessary phase distribution to all dipoles of the antenna. All dimensions of the antenna follow the
(1)τ=Lx-1Lx=Sx-1Sx=Wx-1Wx,
where Lx is the length of the dipole “x”, Wx is the width of the dipole “x” and Sx is the separation between the dipole “x”, and the dipole “x-1”. The dipole length is associated with the work frequency, the dipole width with the dipole impedance and the separations between dipoles is associated with the coupling between neighbouring dipoles. The feed line width is adjusted for a 50 Ω impedance at the feed point. The optimal behaviour of the log-periodic antenna is achieved when the periodic relationship between dimensions is τ=0.88 [13].Figure 6
Log-periodic antenna scheme.The log-periodic antenna proposed consists of 6 dipoles, with the bigger dipole designed for a work frequency of 1.2 GHz and the small dipole designed for 2.58 GHz. As dielectric substrate, a piece of low-cost FR4 substrate was used. The final dimensions, optimized with a parametric study carried out with the 3D-FDTD algorithm [12], are summarized in Table 2. The fabricated prototype is show in Figure 7.Table 2
Log-periodic antenna dimensions (τ=0.88).
L1 = 48.8 mmL2 = 55.5 mmL3 = 63 mmL4 = 71.6 mmL5 = 81.4 mmL6 = 92.5 mmS1 = 38.3 mmS2 = 24.4 mmS3 = 27.7 mmS4 = 31.5 mmS5 = 35.8 mmS6 = 40.7 mmW1 = 1.6 mmW2 = 1.8 mmW3 = 2.04 mmW4 = 2.32 mmW5 = 2.64 mmW6 = 3 mmWL = 3 mmFigure 7
Fabricated prototype of the log-periodic antenna (ruler in cm).The measured and simulated return losses are presented in Figure8, with a good agreement between both results within the whole frequency range studied. As observed, for VSWR <2 (S11<10) two frequency bands are obtained. This dual behaviour instead of a wide-band feature is due to the electric coupling between dipoles and is typical in these log-periodic antennas when the number of dipoles increases [13]. The central frequency of the first frequency band is 1.34 GHz (measured results) with a bandwidth of 430 MHz. The second frequency band is centred at 2.14 GHz and the bandwidth is around 1 GHz.Figure 8
Simulated and measured return losses of the log-periodic antenna.In Figure9, we present the measured and simulated radiation patterns of the antenna at the central frequency of the two bands and for the principal planes. A slightly directive behaviour is observed, especially at the second frequency band, with the maximum of radiation towards the feed point. The measured gain was 4.8 dBi for the central frequency of the first band and around 0 dBi for 2.2 GHz.Simulated and measured radiation patterns of the log-periodic antenna.
(a)
E plane 1.4 GHz(b)
H plane 1.4 GHz(c)
E plane 2.2 GHz(d)
H plane 2.2 GHzFinally, the electric field distributionEy component in the middle point of the dielectric substrate is calculated from the time domain electric and magnetic fields. The results for the central frequency of both frequency bands of the log-periodic antenna are presented in Figure 10. The estimated antenna efficiency was about 90% for the low-frequency band and about 83% for the high-frequency band.Field distribution of the log-periodic antenna.
(a)
1.4 GHz(b)
2.2 GHz


## 2.1. Yagi-Like Antenna

This antenna is proposed for open field wireless sensor networks applications at the free license 868 MHz band. In a particular application [10], some weather stations are located in different and remote places in a wide region (10 × 10 km2). For far end-node stations, standard directive Yagi-Uda antennas are normally used. Printed antennas are proposed as a good alternative for this kind of applications, because their low price and the possibility of integration with the nonmetallic box of the electric sensing devices.The scheme of the Yagi-like antenna is shown in Figure1. The antenna consists on a dipole with the arms located in both sides of the dielectric substrate and a number of director elements with the same dimensions. The dipole is fed by a strip line printed on both sides of the substrate. This scheme of the driver provides the necessary electrical phase to each arm of the dipole, without external elements, allowing a reduction of the final size of the antenna. At the bottom side of the dielectric substrate a truncated ground plane is located. This ground plane acts as reflector element of the antenna [11].Figure 1
Yagi-like antenna scheme.The dipole length is slightly smaller thanλ/2 at the work frequency and the other dimensions of the antenna are obtained by parametric simulations with our 3D-FDTD algorithm [12].The Yagi-like printed antenna is designed for an 868 MHz frequency work onto a piece of low-cost FR4 substrate. Due to final size of the Yagi-like antenna at this low frequency, only two director elements are considered. The optimized dimensions of the antenna are summarized in Table1. In Figure 2 we show the fabricated prototype of the Yagi-like antenna.Table 1
Yagi-like antenna dimensions for 868 MHz.
LDIP = 124.1 mmDDIP = 69.1 mmLDIR = 101.5 mmDDIR = 69.1 mmw = 3.2 mmLM = 180 mmWM = 42.3 mmFigure 2
Fabricated prototype of the 868 MHz Yagi-like antenna (ruler in cm).The measured and calculated return losses are presented in Figure3. A good agreement between both results is obtained, with a measured bandwidth of 138 MHz, around 15% of the central frequency.Figure 3
Simulated and measured return losses of the 868 MHz Yagi-like antenna.The measured and calculated normalized radiation patterns of the Yagi-like antenna for the principal planes at 868 MHz are presented in Figure4. As observed, the antenna displays a directive behaviour with a measured gain of 7 dBi. The estimated antenna efficiency was around 92%.Simulated and measured radiation patterns of the 868 MHz Yagi-like antenna.
(a)
E plane(b)
H planeIn Figure5 we show the normalized electric field distribution Ey component in the middle point of the dielectric substrate at 868 MHz. It is well appreciated that the antenna is fed with the correct phase at the operation frequency.Figure 5
Field distribution of the 868 MHz Yagi-like antenna.


## 2.2. Log-Periodic Antenna

In this paragraph we focus on a wider band design. The range of application of such antennas is well stated [13]. Our particular design includes the L-band and the standard Wi-Fi band, as an example of integrating both technologies.The antenna scheme is shown in Figure6. The antenna consists of a number of printed dipoles with the arms printed in both sides of the dielectric substrate alternatively. Shorter dipoles are located close to the feed point. A strip line printed on both sides of the substrate is used to feed all dipoles. This scheme provides the necessary phase distribution to all dipoles of the antenna. All dimensions of the antenna follow the
(1)τ=Lx-1Lx=Sx-1Sx=Wx-1Wx,
where Lx is the length of the dipole “x”, Wx is the width of the dipole “x” and Sx is the separation between the dipole “x”, and the dipole “x-1”. The dipole length is associated with the work frequency, the dipole width with the dipole impedance and the separations between dipoles is associated with the coupling between neighbouring dipoles. The feed line width is adjusted for a 50 Ω impedance at the feed point. The optimal behaviour of the log-periodic antenna is achieved when the periodic relationship between dimensions is τ=0.88 [13].Figure 6
Log-periodic antenna scheme.The log-periodic antenna proposed consists of 6 dipoles, with the bigger dipole designed for a work frequency of 1.2 GHz and the small dipole designed for 2.58 GHz. As dielectric substrate, a piece of low-cost FR4 substrate was used. The final dimensions, optimized with a parametric study carried out with the 3D-FDTD algorithm [12], are summarized in Table 2. The fabricated prototype is show in Figure 7.Table 2
Log-periodic antenna dimensions (τ=0.88).
L1 = 48.8 mmL2 = 55.5 mmL3 = 63 mmL4 = 71.6 mmL5 = 81.4 mmL6 = 92.5 mmS1 = 38.3 mmS2 = 24.4 mmS3 = 27.7 mmS4 = 31.5 mmS5 = 35.8 mmS6 = 40.7 mmW1 = 1.6 mmW2 = 1.8 mmW3 = 2.04 mmW4 = 2.32 mmW5 = 2.64 mmW6 = 3 mmWL = 3 mmFigure 7
Fabricated prototype of the log-periodic antenna (ruler in cm).The measured and simulated return losses are presented in Figure8, with a good agreement between both results within the whole frequency range studied. As observed, for VSWR <2 (S11<10) two frequency bands are obtained. This dual behaviour instead of a wide-band feature is due to the electric coupling between dipoles and is typical in these log-periodic antennas when the number of dipoles increases [13]. The central frequency of the first frequency band is 1.34 GHz (measured results) with a bandwidth of 430 MHz. The second frequency band is centred at 2.14 GHz and the bandwidth is around 1 GHz.Figure 8
Simulated and measured return losses of the log-periodic antenna.In Figure9, we present the measured and simulated radiation patterns of the antenna at the central frequency of the two bands and for the principal planes. A slightly directive behaviour is observed, especially at the second frequency band, with the maximum of radiation towards the feed point. The measured gain was 4.8 dBi for the central frequency of the first band and around 0 dBi for 2.2 GHz.Simulated and measured radiation patterns of the log-periodic antenna.
(a)
E plane 1.4 GHz(b)
H plane 1.4 GHz(c)
E plane 2.2 GHz(d)
H plane 2.2 GHzFinally, the electric field distributionEy component in the middle point of the dielectric substrate is calculated from the time domain electric and magnetic fields. The results for the central frequency of both frequency bands of the log-periodic antenna are presented in Figure 10. The estimated antenna efficiency was about 90% for the low-frequency band and about 83% for the high-frequency band.Field distribution of the log-periodic antenna.
(a)
1.4 GHz(b)
2.2 GHz


## 3. Conclusions

Microstrip printed technology can be used for the design of good performing antennas for frequencies below 2.45 GHz. Due to the lesser losses at lower frequencies, low cost substrates can be considered. In addition, for dipole based designs, the electromagnetic field mainly travels through the air. This fact helps to have good efficiencies and acceptable overall antenna sizes. This way, antennas for the proposed purposes can be fabricated in a DIN A4 standard sheet of common printed circuit board (PCB) such as FR4. Successful designs have been demonstrated for a Yagi-like antenna for wireless sensor network deployment (ISM band at 868 MHz) and a log-periodic dipole printed antenna for wide band applications. The efficiency in all cases was around 90%, keeping good electrical (S11) and radiation parameters.



---

*Source: 612170-2012-04-02.xml*