“…However, the dimensions also can be analyzed from the transmission line model, TM (Transverse Magnetic Wave) mode [26]. Basically, in the TM mode model, the rectangular patch dimensions are calculated as in Equation (1) to Equation (3) [1], w=c2fεr+12,εeff=12(εr+1)+12(εr−1)[11+12(tsubw)],l=c2fεeff−0.824tsub((εeff+0.3)(wtsub+0.264)(εeff−0.258)(wtsub+0.8)), where c is ...…”
Section: Methodsmentioning
confidence: 99%
“…However, the dimensions also can be analyzed from the transmission line model, TM (Transverse Magnetic Wave) mode [ 26 ]. Basically, in the TM mode model, the rectangular patch dimensions are calculated as in Equation (1) to Equation (3) [ 1 ], where c is the speed of light (3 × 10 8 m/s), f is the operating frequency, and ε eff is the effective ε r index of the substrate. This model shows good physical insight, but is less accurate.…”
Section: Methodsmentioning
confidence: 99%
“…In recent years, there has been a growing interest from both academia and industry in the deployment of energy capture of ambient energy for fully autonomous powering of microdevices, using different energy harvesting techniques. These microdevices, such as sensors, actuators and so on, are extensively utilized in various daily life applications such as in wearable devices, batteryless remote controls, structural healthcare and agriculture monitoring systems, the Internet of Things (IoT), and so on [ 1 , 2 , 3 ], in which low power consumption is highly demanded. Conventionally, energy supplies for these devices are powered by chemical batteries.…”
Section: Introductionmentioning
confidence: 99%
“…An antenna is the first and the most important element of the RF energy harvesting system, and it affects the amount of captured energy from the environment [ 4 ]. Numerous research works have been reported on the antenna for RF energy harvesting purposes to achieve appropriate characteristics, such as high efficiency [ 11 , 12 , 13 ], lower return loss [ 1 , 14 , 15 ] and an omnidirectional radiation pattern with high gain [ 11 , 12 , 16 ].…”
Section: Introductionmentioning
confidence: 99%
“…Most of the reported materials for the antennas designed for RF energy harvesting are made of conventional printed circuit board (PCB)-based materials such as Rogers, RT/Duroid and FR4 substrates [ 1 , 11 , 14 , 17 ], which is due to the established fabrication concepts from many years ago, low cost, easy fabrication and easily available material.…”
This paper investigates micromachined antenna performance operating at 5 GHz for radio frequency (RF) energy harvesting applications by comparing different substrate materials and fabrication modes. The research aims to discover appropriate antenna designs that can be integrated with the rectifier circuit and fabricated in a CMOS (Complementary Metal-Oxide Semiconductor)-compatible process approach. Therefore, the investigation involves the comparison of three different micromachined antenna substrate materials, including micromachined Si surface, micromachined Si bulk with air gaps, and micromachined glass-surface antenna, as well as conventional RT/Duroid-5880 (Rogers Corp., Chandler, AZ, USA)-based antenna as the reference. The characteristics of the antennas have been analysed using CST-MWS (CST MICROWAVE STUDIO®—High Frequency EM Simulation Tool). The results show that the Si-surface micromachined antenna does not meet the parameter requirement for RF antenna specification. However, by creating an air gap on the Si substrate using a micro-electromechanical system (MEMS) process, the antenna performance could be improved. On the other hand, the glass-based antenna presents a good S11 parameter, wide bandwidth, VSWR (Voltage Standing Wave Ratio) ≤ 2, omnidirectional radiation pattern and acceptable maximum gain of >5 dB. The measurement results on the fabricated glass-based antenna show good agreement with the simulation results. The study on the alternative antenna substrates and structures is especially useful for the development of integrated patch antennas for RF energy harvesting systems.
“…However, the dimensions also can be analyzed from the transmission line model, TM (Transverse Magnetic Wave) mode [26]. Basically, in the TM mode model, the rectangular patch dimensions are calculated as in Equation (1) to Equation (3) [1], w=c2fεr+12,εeff=12(εr+1)+12(εr−1)[11+12(tsubw)],l=c2fεeff−0.824tsub((εeff+0.3)(wtsub+0.264)(εeff−0.258)(wtsub+0.8)), where c is ...…”
Section: Methodsmentioning
confidence: 99%
“…However, the dimensions also can be analyzed from the transmission line model, TM (Transverse Magnetic Wave) mode [ 26 ]. Basically, in the TM mode model, the rectangular patch dimensions are calculated as in Equation (1) to Equation (3) [ 1 ], where c is the speed of light (3 × 10 8 m/s), f is the operating frequency, and ε eff is the effective ε r index of the substrate. This model shows good physical insight, but is less accurate.…”
Section: Methodsmentioning
confidence: 99%
“…In recent years, there has been a growing interest from both academia and industry in the deployment of energy capture of ambient energy for fully autonomous powering of microdevices, using different energy harvesting techniques. These microdevices, such as sensors, actuators and so on, are extensively utilized in various daily life applications such as in wearable devices, batteryless remote controls, structural healthcare and agriculture monitoring systems, the Internet of Things (IoT), and so on [ 1 , 2 , 3 ], in which low power consumption is highly demanded. Conventionally, energy supplies for these devices are powered by chemical batteries.…”
Section: Introductionmentioning
confidence: 99%
“…An antenna is the first and the most important element of the RF energy harvesting system, and it affects the amount of captured energy from the environment [ 4 ]. Numerous research works have been reported on the antenna for RF energy harvesting purposes to achieve appropriate characteristics, such as high efficiency [ 11 , 12 , 13 ], lower return loss [ 1 , 14 , 15 ] and an omnidirectional radiation pattern with high gain [ 11 , 12 , 16 ].…”
Section: Introductionmentioning
confidence: 99%
“…Most of the reported materials for the antennas designed for RF energy harvesting are made of conventional printed circuit board (PCB)-based materials such as Rogers, RT/Duroid and FR4 substrates [ 1 , 11 , 14 , 17 ], which is due to the established fabrication concepts from many years ago, low cost, easy fabrication and easily available material.…”
This paper investigates micromachined antenna performance operating at 5 GHz for radio frequency (RF) energy harvesting applications by comparing different substrate materials and fabrication modes. The research aims to discover appropriate antenna designs that can be integrated with the rectifier circuit and fabricated in a CMOS (Complementary Metal-Oxide Semiconductor)-compatible process approach. Therefore, the investigation involves the comparison of three different micromachined antenna substrate materials, including micromachined Si surface, micromachined Si bulk with air gaps, and micromachined glass-surface antenna, as well as conventional RT/Duroid-5880 (Rogers Corp., Chandler, AZ, USA)-based antenna as the reference. The characteristics of the antennas have been analysed using CST-MWS (CST MICROWAVE STUDIO®—High Frequency EM Simulation Tool). The results show that the Si-surface micromachined antenna does not meet the parameter requirement for RF antenna specification. However, by creating an air gap on the Si substrate using a micro-electromechanical system (MEMS) process, the antenna performance could be improved. On the other hand, the glass-based antenna presents a good S11 parameter, wide bandwidth, VSWR (Voltage Standing Wave Ratio) ≤ 2, omnidirectional radiation pattern and acceptable maximum gain of >5 dB. The measurement results on the fabricated glass-based antenna show good agreement with the simulation results. The study on the alternative antenna substrates and structures is especially useful for the development of integrated patch antennas for RF energy harvesting systems.
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