# A Dual-Band Antenna for RF Energy Harvesting Systems in Wireless Sensor Networks

Authors: A. Bakkali; J. Pelegri-Sebastia; T. Sogorb; V. Llario; A. Bou-Escriva
Journal: Journal of Sensors
 (2016)

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## Abstract

In this paper, we focus on ambient radio frequency energy available from commercial broadcasting stations in order to provide a system based on RF energy harvesting using a new design of receiving antenna. Several antenna designs have been proposed for use in RF energy harvesting systems, as a pertinent receiving antenna design is highly required since the antenna features can affect the amount of energy harvested. The proposed antenna is aimed at greatly increasing the energy harvesting efficiency over Wi-Fi bands: 2.45 GHz and 5 GHz. This provides a promising alternative energy source in order to power sensors located in harsh environments or remote places, where other energy sources are impracticable. The dual-band antenna can be easily integrated with RF energy harvesting system on the same circuit board. Simulations and measurements were carried out to evaluate the antenna performances and investigate the effects of different design parameters on the antenna performance. The receiving antenna meets the required bandwidth specification and provides peak gain of more than 4 dBi across the operating band.


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## Body

## 1. Introduction

The use of renewable energies to power electronics devices is not a new concept. The process of extracting energy from the ambient environment to generate electricity is termed as energy harvesting or energy scavenging [1, 2]. This energy can be harvested from various sources available in the ambient environment such as thermal energy [3, 4], mechanical energy [5], and radiant energy [6, 7]. In Table 1, properties of widely utilized ambient energy sources are introduced.Table 1
Characteristics of various energy sources and harvested power.
Source
Source power
Harvested power
Ambient light
Indoor
0.1 mW/cm2
10μW/cm2
Outdoor
100 mW/cm2
10 mW/cm2
Vibration
Human
0.5 m @ 1 Hz 1 m/s2 @ 50 Hz
4μW/cm2
Industrial
1 m @ 5 Hz 10 m/s2 @ 1 kHz
100μW/cm2
Thermal energy
Human
20 mW/cm2
30μW/cm2
Industrial
100 mW/cm2
1–10 mW/cm2
RF
Cell phone
0.3μW/cm2
0.1μW/cm2Among the available ambient energy sources, RF energy has greatly grown due to the preponderance of wireless signals, such as mobile base stations [8] and Wi-Fi networks [9], radio and TV transmitters [10–12], and microwave radios and mobile phones [13]. Compared to the other energy sources, RF energy provides a relatively low energy density of 0.2 nW/cm2–1 μW/cm2. Energy harvesters for low power devices, including applications related to wireless sensor networks (WSNs), extend significantly the operating lifetime and present a new challenge as the harvesting system has to be comparable in size with sensor nodes. This technique could be especially useful for powering up the wireless networks deployed in harsh environment, charging batteries, or storing energy in super capacitors. In this paper, we focus on ambient RF energy harvesting technology that will have an important potential to impact sensors located in harsh environments or remote places, where other energy sources as wind or solar sources are impracticable. This technique attracted significant attention and multiple RF energy harvesting systems including receiving antennas, matching circuits, and rectifying circuits which have been developed for green supply of low consumption electronics [14, 15]. The general structure of a typical RF energy harvester is shown in Figure 1, comprised of receiving antenna along with a circuit capable of converting RF signals into DC voltage. The antenna picks up the RF power sent out by the network controller, the impedance matching network ensures maximum power transfer in the system, and the rectifier converts the RF power to a DC voltage.Figure 1
Block diagram of RF energy harvesting system.The components of the energy harvesting system (antenna, matching network, and rectifier) are usually known as a Rectenna or a RF/DC, which is able to harvest high-frequency energy in free space and convert it to DC power. Harvesting ambient RF energy and converting the harvested power to useful DC power require a careful design:(i)
An efficient antenna for maximizing the reception of the ambient RF signals.(ii)
A matching network to match the antenna impedance with the complex load impedance, composed of inductive and capacitive elements, in order to achieve the maximum power delivery from antenna to rectifier.(iii)
Optimization of the rectifier circuit for RF to DC conversion.In literature numerous research works have been reported on ambient RF energy harvesting systems. The authors in [16] presented an optimized wireless energy harvester for an UHF digital TV signal. The power harvested at distance of over 6.3 km from the TV broadcast source is successfully used to power and sustain a 16-bit embedded microcontroller for sensing and machine-to-machine applications without the use of batteries. In [17], the authors proposed a multiband RF energy harvesting system for three different operating frequencies, 900 MHz, 1800 MHz, and 2.45 GHz. The proposed system can achieve 15% more efficiency compared to single-frequency RF harvester. However, in [18], the RF energy harvesting system was designed based on planar dual-band antenna at 900 and 2000 MHz that can provide the required impedance matching to the RF chip at two bands and can be easily integrated with the RF harvester chip on the same circuit board. The authors in [19] proposed a prototype microstrip patch antenna to operate in the 2.4 GHz ISM band in order to collect RF energy and charge a super capacitor to power a sensor node to 3.6 V in 27 s for structural health monitoring applications. A triple-band antenna for ambient RF energy harvesting system operating at 940 MHz, 1.95 GHz, and 2.44 GHz is designed in [20] with new technique for multiple-band matching of a rectifier to achieve high efficiency. The realized gain is 0.3 dBi, 2.3 dBi, and 3.5 dBi, respectively, and the measured received power from harvesting RF energy at three bands simultaneously is 6.6 times more than that at single 900 MHz band. Authors in [21] present a novel RF energy harvesting system for energizing the WSN. The novelty of the work is the use of the multiband microstrip crossed monopole antenna with circular polarization and impedance of 377 Ω. Achieved results show that the rectifying antenna system generates the desired voltage to energize the wireless sensor nodes. Table 2 summarizes the features of some energy harvesting antennas from various RF energy sources proposed in literature.Table 2
Overview of RF harvesting energy antenna.
Type of antenna
Frequency
Maximum voltage
Maximum performance
Energy harvested
Reference
Folded patch antennaMaximum power received is −10 dBm
2.4 GHz
n/a
n/a
373,248μW
[22]
Spiral antennaMaximum power received is −42 dBm
2.4 GHz
n/a
0.60%
400 pW
[23]
Patch antenna
500–700 MHz
134 mV
18.2%(Pin = −20 dBm)
n/a
[24]
Loop antenna
954 kHz
520 mV
n/a
60.4μJ
[25]In this paper, a novel dual-band antenna is designed operating at Wi-Fi bands 2.45 GHz and 5 GHz and is presented in order to harvest successfully RF power. Section2 describes the proposed dual-band antenna considered for collecting RF energy. Section 3 discusses the measured results and the antenna performance. Finally, conclusions are drawn in Section 4.


## 2. RF Energy Harvesting Antenna Design

This section deals with the design of dual-band antenna for maximizing RF signal harvested. The simulated results and analysis for the energy harvesting antenna are discussed.


### 2.1. Antenna Design

The geometry of the proposed antenna is shown in Figure2. The substrate material is RT/Duroid 5870 [26] as one of the popular industry-wide standard substrate material formats for electronic circuit boards. The key property of RT/Duroid 5870 relates to the dielectric permittivity constancy over a wide frequency range and its low dissipation factor that extends its usefulness to Ku-band and above. The important specifications chosen in simulation for this design are as follows: the thickness of substrate, 1.6 mm; the thickness of copper, 0.035 mm; the relative permittivity, 2.33; and the loss tangent, 0.0012. Duroid 5870 has lower loss tangent of 0.0012 compared to 0.02 for FR4. The antenna size is characterized by its length, width, and height (L, W, and h) and is fed by feed line and is followed by a ground plane. The antenna is designed and optimized to capture the energy from the ambient at radio frequency range of Wi-Fi bands 2.45 GHz and 5 GHz. The challenge is to design an antenna able to operate in both 2.4 GHz band and 5 GHz band. This antenna is highly desired also for the system flexibility.Figure 2
Geometry of the proposed dual-band antenna.The antenna design required the best choice of the substrate dielectric constant, length and width of the antenna, and the ground plane. The properties and performance of the proposed antenna have been predicted and optimized through electromagnetic simulation software in Ansoft HFSS environment. The size of the proposed RF energy harvester can be reduced by miniaturizing the antenna. An antenna is one of the few components, the size of which is related to the operating frequency. In general, microstrip antennas are half-wavelength structures, with a resonant frequency given by (1) [27], where C is the speed of light, L is the patch length of the antenna, and εr is the relative permittivity of the grounded microwave substrate. The dielectric constant of the substrate has a considerable role in the antenna overall performance, the width, the length, and the resonant frequency. Consider(1)f=C2∗Lεr.


### 2.2. Simulations Results

With the overall objective of RF efficient energy harvesting, we focused on the development, fabrication, and characterization of a dual-band antenna designed to serve as our receiving antenna. The reflection coefficient of the proposed antenna is measured between 1 GHz and 6 GHz. The simulations result of the return loss (S11) is shown in Figure 3. From the result it is observed that the antenna is resonating at 2.47 GHz, 4.93 GHz, and 5.69 GHz with return loss below 14 dB.Figure 3
Simulated return lossS11 (dB) versus frequency (GHz).The results of the simulated impedance are shown in Figure4. The real part of the impedance at the resonant frequencies is close to 50 Ω, (m1) 44.33 Ω, and (m3) 52.76 Ω for 2.4 GHz and 5.69 GHz, respectively. The imaginary part of the impedance is almost negligible in the desired range of frequency band.Figure 4
Simulated input impedance of antenna.Figure5 presents the peak gain of the proposed dual-band antenna. In the 2.4 GHz band, the peak gain is about 4 dBi, while in the 5 GHz band the peak gain is around 7 dBi. A high antenna gain is also required to harvest as much wireless power as possible, especially in the case when the source location is known. The radiation characteristics of the proposed antenna as distributions of the energy radiated in the space are shown in Figure 6. The shape of radiation varies according to frequency; a quasi-omnidirectional radiation is obtained in 2.4 GHz and 5 GHz frequencies. Therefore, the antenna designed is very interesting for a system of wireless energy harvesting, meeting the desired criteria to maximize the captured RF energy.Figure 5
Peak gain of the proposed dual-band antenna.Figure 6
3D radiation pattern of the antenna at 2.4 GHz (a) and 5 GHz (b).
(a)
(b)The results obtained are very interesting and indicate clearly that the proposed antenna is capable of providing good performances in terms of return loss, gain, and radiation pattern. Experimental tests in order to characterize the performance of the proposed antenna will be discussed in Section3.


## 2.1. Antenna Design

The geometry of the proposed antenna is shown in Figure2. The substrate material is RT/Duroid 5870 [26] as one of the popular industry-wide standard substrate material formats for electronic circuit boards. The key property of RT/Duroid 5870 relates to the dielectric permittivity constancy over a wide frequency range and its low dissipation factor that extends its usefulness to Ku-band and above. The important specifications chosen in simulation for this design are as follows: the thickness of substrate, 1.6 mm; the thickness of copper, 0.035 mm; the relative permittivity, 2.33; and the loss tangent, 0.0012. Duroid 5870 has lower loss tangent of 0.0012 compared to 0.02 for FR4. The antenna size is characterized by its length, width, and height (L, W, and h) and is fed by feed line and is followed by a ground plane. The antenna is designed and optimized to capture the energy from the ambient at radio frequency range of Wi-Fi bands 2.45 GHz and 5 GHz. The challenge is to design an antenna able to operate in both 2.4 GHz band and 5 GHz band. This antenna is highly desired also for the system flexibility.Figure 2
Geometry of the proposed dual-band antenna.The antenna design required the best choice of the substrate dielectric constant, length and width of the antenna, and the ground plane. The properties and performance of the proposed antenna have been predicted and optimized through electromagnetic simulation software in Ansoft HFSS environment. The size of the proposed RF energy harvester can be reduced by miniaturizing the antenna. An antenna is one of the few components, the size of which is related to the operating frequency. In general, microstrip antennas are half-wavelength structures, with a resonant frequency given by (1) [27], where C is the speed of light, L is the patch length of the antenna, and εr is the relative permittivity of the grounded microwave substrate. The dielectric constant of the substrate has a considerable role in the antenna overall performance, the width, the length, and the resonant frequency. Consider(1)f=C2∗Lεr.


## 2.2. Simulations Results

With the overall objective of RF efficient energy harvesting, we focused on the development, fabrication, and characterization of a dual-band antenna designed to serve as our receiving antenna. The reflection coefficient of the proposed antenna is measured between 1 GHz and 6 GHz. The simulations result of the return loss (S11) is shown in Figure 3. From the result it is observed that the antenna is resonating at 2.47 GHz, 4.93 GHz, and 5.69 GHz with return loss below 14 dB.Figure 3
Simulated return lossS11 (dB) versus frequency (GHz).The results of the simulated impedance are shown in Figure4. The real part of the impedance at the resonant frequencies is close to 50 Ω, (m1) 44.33 Ω, and (m3) 52.76 Ω for 2.4 GHz and 5.69 GHz, respectively. The imaginary part of the impedance is almost negligible in the desired range of frequency band.Figure 4
Simulated input impedance of antenna.Figure5 presents the peak gain of the proposed dual-band antenna. In the 2.4 GHz band, the peak gain is about 4 dBi, while in the 5 GHz band the peak gain is around 7 dBi. A high antenna gain is also required to harvest as much wireless power as possible, especially in the case when the source location is known. The radiation characteristics of the proposed antenna as distributions of the energy radiated in the space are shown in Figure 6. The shape of radiation varies according to frequency; a quasi-omnidirectional radiation is obtained in 2.4 GHz and 5 GHz frequencies. Therefore, the antenna designed is very interesting for a system of wireless energy harvesting, meeting the desired criteria to maximize the captured RF energy.Figure 5
Peak gain of the proposed dual-band antenna.Figure 6
3D radiation pattern of the antenna at 2.4 GHz (a) and 5 GHz (b).
(a)
(b)The results obtained are very interesting and indicate clearly that the proposed antenna is capable of providing good performances in terms of return loss, gain, and radiation pattern. Experimental tests in order to characterize the performance of the proposed antenna will be discussed in Section3.


## 3. Fabrication and Evaluation

### 3.1. Measured Results

The fundamental objective of this research has been to develop a receiving antenna for wireless energy harvesting for the purpose of powering the wireless sensor networks. In order to validate the simulated results, a prototype of the proposed antenna was implemented and fabricated on RT/Duroid 5870 substrate (εr=2.33, tan⁡σ=0.0012). Figure 7 shows the prototype antenna realized. The return loss was measured using a Rohde and Schwarz ZVA 24 Vector Network Analyzer and the radiation patterns were tested in the anechoic chambers at the Research Center of Polytechnic University of Valencia.Figure 7
Photograph of proposed antenna (fabricated prototype).Several experimental studies were conducted as part of this research. The first series of experiments were conducted in the laboratory and were designed to compare the performance of our prototype antenna with the simulations results. In order to evaluate the simulation analysis, the antenna prototype was fabricated and tested in the anechoic chamber.


### 3.2. Discussion and Analysis

The measured return loss, shown in Figure8, indicates clearly that the proposed antenna has a multiband characteristic. Two resonant frequencies are located at about 2.4 GHz and 5 GHz, with the return losses reaching 25 dB and 13.5 dB, respectively. Compared with the simulated results, the measured reflection coefficient displays good agreement in resonant frequency and bandwidth. The radiation mechanism of the total electric field is shown in Figure 9 for 2.4 GHz and 5 GHz.Figure 8
Measured return loss (dB).Figure 9
Total electric field of the dual-band antenna at 2.4 GHz and 5 GHz.


### 3.3. RF to DC Power Converter

Appropriate electronic circuitry for impedance matching and rectifier may be available commercially or may require design and fabrication. The proposed RF harvesting system consists of two parts: rectifier and receiving antenna without matching circuit. The RF-DC conversion module is composed of 7 stages. The design of the printed circuit is based on work performed by Din et al. [28]. The printed circuit board of 7-stage RF-DC conversion module for the proposed RF energy harvesting system is shown in Figure 10. The diodes used are SMS7630-079LF RF Schottky Diodes and capacitors of 1.8 nF in terms of capacity. These diodes are low substrate losses and have low forward voltage, very fast switching and have been modeled for energy harvesting circuits.Figure 10
Measurements protocol.Printed circuit board (PCB) was manufactured on FR 4 substrate with thickness of 1.6 mm and dielectric constant of 3.9. Photograph of two assembled circuit board is shown in Figure11. The circuit is performed with the dimensions of 71.6 mm × 12 mm. The main objective is to maximize the DC energy harvested by recovering all Wi-Fi signals available. The overall RF energy harvesting system is designed for energizing low power devices. Measurements are performed under real conditions by using an intentional radio frequency signal source from the Signal Generator R&S SMIQ 04B and a transmission directional antenna operating in 2.4–2.5 GHz with gain of 14 dBi. The test results of the DC output voltage obtained as a function of the signal generator power are shown in Figure 12.Figure 11
Prototypes of the assembled circuit board of 7-stage voltage doubler.Figure 12
Results of test for DC output of proposed system versus input power at a distance of 170 cm.The voltage output decreases with the distance between the transmission antenna and the harvesting energy system as illustrated in Figure13. The system produces DC output voltage of 1.3 V at 10 dBm and a distance of 60 cm from the signal generator.Figure 13
DC output of proposed system versus the distance for a power of 10 dBm.


## 3.1. Measured Results

The fundamental objective of this research has been to develop a receiving antenna for wireless energy harvesting for the purpose of powering the wireless sensor networks. In order to validate the simulated results, a prototype of the proposed antenna was implemented and fabricated on RT/Duroid 5870 substrate (εr=2.33, tan⁡σ=0.0012). Figure 7 shows the prototype antenna realized. The return loss was measured using a Rohde and Schwarz ZVA 24 Vector Network Analyzer and the radiation patterns were tested in the anechoic chambers at the Research Center of Polytechnic University of Valencia.Figure 7
Photograph of proposed antenna (fabricated prototype).Several experimental studies were conducted as part of this research. The first series of experiments were conducted in the laboratory and were designed to compare the performance of our prototype antenna with the simulations results. In order to evaluate the simulation analysis, the antenna prototype was fabricated and tested in the anechoic chamber.


## 3.2. Discussion and Analysis

The measured return loss, shown in Figure8, indicates clearly that the proposed antenna has a multiband characteristic. Two resonant frequencies are located at about 2.4 GHz and 5 GHz, with the return losses reaching 25 dB and 13.5 dB, respectively. Compared with the simulated results, the measured reflection coefficient displays good agreement in resonant frequency and bandwidth. The radiation mechanism of the total electric field is shown in Figure 9 for 2.4 GHz and 5 GHz.Figure 8
Measured return loss (dB).Figure 9
Total electric field of the dual-band antenna at 2.4 GHz and 5 GHz.


## 3.3. RF to DC Power Converter

Appropriate electronic circuitry for impedance matching and rectifier may be available commercially or may require design and fabrication. The proposed RF harvesting system consists of two parts: rectifier and receiving antenna without matching circuit. The RF-DC conversion module is composed of 7 stages. The design of the printed circuit is based on work performed by Din et al. [28]. The printed circuit board of 7-stage RF-DC conversion module for the proposed RF energy harvesting system is shown in Figure 10. The diodes used are SMS7630-079LF RF Schottky Diodes and capacitors of 1.8 nF in terms of capacity. These diodes are low substrate losses and have low forward voltage, very fast switching and have been modeled for energy harvesting circuits.Figure 10
Measurements protocol.Printed circuit board (PCB) was manufactured on FR 4 substrate with thickness of 1.6 mm and dielectric constant of 3.9. Photograph of two assembled circuit board is shown in Figure11. The circuit is performed with the dimensions of 71.6 mm × 12 mm. The main objective is to maximize the DC energy harvested by recovering all Wi-Fi signals available. The overall RF energy harvesting system is designed for energizing low power devices. Measurements are performed under real conditions by using an intentional radio frequency signal source from the Signal Generator R&S SMIQ 04B and a transmission directional antenna operating in 2.4–2.5 GHz with gain of 14 dBi. The test results of the DC output voltage obtained as a function of the signal generator power are shown in Figure 12.Figure 11
Prototypes of the assembled circuit board of 7-stage voltage doubler.Figure 12
Results of test for DC output of proposed system versus input power at a distance of 170 cm.The voltage output decreases with the distance between the transmission antenna and the harvesting energy system as illustrated in Figure13. The system produces DC output voltage of 1.3 V at 10 dBm and a distance of 60 cm from the signal generator.Figure 13
DC output of proposed system versus the distance for a power of 10 dBm.


## 4. Conclusion

RF energy harvesting is a key technology due to its potential to provide power indefinitely. It is a green technology suitable for a wide range of wireless applications such as RFID tags, implantable electronics devices, and wireless sensor networks. In this paper, a novel receiving antenna capable of dual-band operation has been proposed for RF energy harvesting system. A dual-band with wide bandwidth characteristics is observed which covers Wi-Fi bands. The results obtained indicate a good overall performance of the proposed antenna at the required frequency range: return loss better than 20 dB with impedance close to 50 Ω and quasi-omnidirectional radiation patterns. Good agreements are achieved between the simulated and measured results that satisfy the end application requirement. Based on the results achieved the current work consists in improving the antenna performances in order to cover completely the required bandwidths of IEEE 802.11b/g and IEEE 802.11a. The patch antenna is especially suitable for narrow bandwidth applications. Therefore, the challenge is to expand the bandwidth in order to make the antenna for wideband energy harvesting environment.



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