Design of a Rectenna in 2.45 GHz Band Frequency for Energy Harvesting ()
1. Introduction
The low-energy electronic devices or connected objects manufacturing industry have experienced growth in production in recent years. This growth has led to the implementation and further development of ambient energy recovery systems [1] [2] [3] [4] [5], including radiofrequency (RF) energy harvesting systems. The development of RF energy harvesting systems has been made possible by the permanent presence of electromagnetic waves or radio waves in the ambient environment. These waves are produced by television and radio stations, Wi-Fi access points, access networks of fixed and mobile telephone operators. One source of energy that is easily obtained is an access point (Wi-Fi). RF systems consist mainly of a rectenna which is an assembly of receiving antenna and rectifier. The receiving antenna picks up the radio signal from the source and converts it into an electrical signal. This electrical signal is then routed through a rectifier which converts it into Direct Current (DC). Microstrip antennas or patch antennas not only considerably allow to reducing the size of the antenna structure, but they are also mechanically robust. Several techniques are developed to design microstrip antennas such as the creation of slots on the radiating element of the antenna. The slots with fractal geometry allowed to increase the bandwidth and the antenna adaptation characteristics [6] [7] [8]. The design of the multiband antenna resulted in a reflection coefficient of −49 dB with a bandwidth of 67 MHz around the resonant frequency of 2400 MHz [8]. A multi-band antenna whose radiated element is loaded with circular, L-shaped, and U-shaped slots is designed [9]. The sensor requires a DC voltage to operate. Therefore, in order to power it from the RF system, it is necessary to convert the electrical signal obtained at the output of the antenna to DC power. Moreover, for maximum power transfer, it is important to associate a matching circuit to this rectifier. Thus, an RF to DC conversion efficiency of 84% was obtained with an L-shaped adapter circuit [10]. For a low input power of 0 dBm a rectifier associated with a stub adaptation network allowed to obtain an efficiency of 62% [6]. The analysis of these works shows that microstrip antennas have a low profile with a low bandwidth around their resonant frequency. To increase this bandwidth, the creation of slots on the radiating element of these antennas is important. Rectifier circuits using fewer diodes help to increase the RF-DC conversion efficiency. In this paper, we proposed a compact rectenna operating at 2.45 GHz band for RF energy harvesting. First, three diamond geometry slots are introduced in the patch antenna design to miniaturize it and make it more efficient. Then, two rectangular slots and one circular slot are added to the radiating element to increase the performance of this antenna. A serial rectifier circuit is used to perform the conversion from RF to DC. In addition, a new L-matching stub network is designed to improve the overall efficiency of the rectenna for low input power.
2. Design and Simulation of the Single Band Antenna
The antenna consists of a rectangular geometry with slots loaded on the radiating element. We used a rectangular patch antenna fed by a microstrip line. Rectangular patch antennas have dimensions that can be calculated from equations whose parameters are related to the characteristics of the substrate, the speed of light in vacuum and the frequency of the antenna [11]. The dimensions of the patch are 32 mm × 42 mm, placed on a Flame Retardant 4 (FR-4) substrate with relative permittivity = 4.4, thickness = 1.6 mm and loss tangent = 0.02. The ground and the radiating element are each 0.035 mm thick. The microstrip feed-line of the antenna has an impedance of 50 Ω. The patch antenna designed by creating diamond-shaped slots on the radiating element is shown in Figure 1. To obtain the frequency band with better performance, we considered the patch antenna shown in Figure 2. The final structure in Figure 2 is obtained by creating new rectangular and circular slots on the patch. The dimensions of this antenna are presented in Table 1. The evaluation of the reflection coefficient as a function of frequency is shown in Figure 3. We can note from Figure 3 the significant improvement of the reflection coefficient with the final antenna structure. We also note an increase in bandwidth. From the initial structure without slots to the secondary structure, we note an increase of 106.33% in bandwidth and 132.29% with the final structure. The bandwidth is therefore 140 MHz around the resonant frequency of 2.45 GHz.
The increase of antenna performance can therefore be explained by the creation of slots on the radiating element.
![]()
Figure 1. Initial (a) second (b) and final (c) structure of the antenna.
![]()
Table 1. Dimensions of the proposed antenna.
![]()
Figure 3. Reflection coefficient variation from initial to final structure.
![]()
Table 2. Results of the reflection coefficient (S11) and gain as a function of frequencies.
Small current flows would have appeared on the radiating element by the presence of slots [6]. This would have led to an increase in the bandwidth and an improvement in the reflection coefficient. Table 2 shows a comparative study of the three antenna structures. From this table, we also note an improvement of the antenna gain with the final antenna structure. We can deduct from Table 2 that the creation of slots also increases the antenna gain. The realized gain variation of the final antenna structure is shown in Figure 4. At the resonance frequency of 2.45 GHz, we obtain a realized gain of 3.48 dB.
The simulated radiation pattern of the antenna at 2.45 GHz frequencies is plotted in Figure 5. The 2 D radiation pattern shows that antenna has an omnidirectional characteristic in the H-plane.
The comparison of our work with others illustrated in Table 3 shows that the
![]()
Figure 5. Radiation patterns of the antenna at 2.45 GHz.
![]()
Table 3. Comparison between our design and others works.
designed and simulated antenna has good performances with a better reflection coefficient at a frequency of 2.45 GHz. The comparative study shows also that the designed antenna has the best reflection coefficient. This indicates that the antenna is highly resonant. This results in a very low signal loss between the antenna and the feed line.
3. Rectifying Circuit Design
The rectifier circuit converts the incoming RF signal received by the antenna into a usable DC voltage for low power applications such as sensors. The topology of the serial rectifier circuit has been chosen.
The selected Schottky diode is the HSMS 2850 type with a series resistance of 25 Ω, a low threshold voltage of 0.25 V and a junction capacitance of 0.18 pF [7]. The matching circuit consists of microstrip lines and inductors. Figure 6 illustrates the design of the rectifier and adapter circuit under ADS. The complex impedance of the antenna ZSource is 48-j × 0.3 Ohm and that of the load Zload is 1 KΩ. The power levels before and after the rectifier circuits are represented in Figure 7. It represents the voltage variations as a function of the frequencies of the source where vin and VOUT are respectively the input and output voltage in the rectifier. We, therefore, note the transfer of direct current power at the output of the rectifier. Figure 7 shows also that the input voltage to the converter can reach a maximum value of 2 dBm which is obtained at 2.45 GHz. This proves that this device is suitable for low input voltages. The conversion efficiency η at the rectifier terminals can be obtained by the relation (1) [8],
(1)
where VL (Volt) is the voltage on the resistor; RL is the resistance value (1 KΩ) and P is input power (Watt) of receiving antenna. P can be computed according
![]()
Figure 6. Simulation of the adaptation and rectification circuit.
![]()
Figure 7. (a) Input Spectrum power; (b) Output Spectrum power.
![]()
Figure 8. Single band rectifier: RF-to-dc conversion efficiency versus input power (dBm).
to Friis transmission equation [6] as:
(2)
where λ is the wavelength of operating frequency, Gt and Gr are respectively the gain of the transmitting antenna and receiving antenna, Pt is the transmitting power, r is the distance between the two antennas. Figure 8 shows the RF-DC conversion efficiency. An efficiency of 54% is therefore achieved for an input power of 0 dBm. However, the maximum power transfer efficiency is 55% with an input power of 3 dBm. This curve also indicates that the conversion system is suitable for low input powers. Figure 9 represents the variation of simulated input and output voltages versus the time for an RF input power of 0 dBm at 2.45 GHz.
The input voltage is sinusoidal while the output voltage is almost constant. We note a higher peak output voltage than the input voltage. The rectifier circuit has therefore not only rectified the input voltage but also amplified it. The designed rectifier gives a maximum output voltage of 732 mV at 2.45 GHz. Table 4 shows a comparative study of the results of the simulation of rectifier circuit
![]()
Figure 9. Simulated input and output voltage.
![]()
Table 4. Comparison with other rectifier circuits.
with other works. We obtained a simple rectifier circuit with a good efficiency at 0 dBm and a fairly high output voltage.
4. Conclusion
In this work, we proposed in the first part a single band antenna for RF energy harvesting operating in the 2.45 GHz frequency band. This antenna is able to recover radio waves from Wi-Fi access points and is compact in size and has good performances at its resonance frequency. In the second part, a rectifier circuit using a single Schottky diode has been designed. Using this single diode rectifier, the power conversion efficiency is simulated and found to be 54% for the antenna at an input power of 0 dBm with a direct rectified voltage of 732 mV. The presented rectenna is suitable for RF energy harvesting at Wi-Fi band.