180-nm CMOS Wideband Capacitor-Free Inductively Coupled Power Receiver and Charger

Wireless microsystems like biomedical implants and embedded sensors derive energy from tiny in-package sources that, unfortunately, exhaust easily, which means that operational life is short. Periodically coupling power wirelessly is one way of replenishing onboard batteries, except that small recei...

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Veröffentlicht in:IEEE journal of solid-state circuits 2013-11, Vol.48 (11), p.2839-2849
Hauptverfasser: Lazaro, Orlando, Rincon-Mora, Gabriel Alfonso
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container_title IEEE journal of solid-state circuits
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creator Lazaro, Orlando
Rincon-Mora, Gabriel Alfonso
description Wireless microsystems like biomedical implants and embedded sensors derive energy from tiny in-package sources that, unfortunately, exhaust easily, which means that operational life is short. Periodically coupling power wirelessly is one way of replenishing onboard batteries, except that small receiver coils suffer from low coupling factors k C and induce low electromotive-force voltages. Today, receivers store and resonate incoming energy between the receiving coil and an off-chip capacitor until the voltage rises sufficiently high for a diode-bridge rectifier to steer power into a battery. The capacitor, however, requires board space and constrains the source to a particular frequency. The 180-nm CMOS power receiver presented in this paper removes the diode bridge, which establishes a minimum voltage below which the system cannot derive power, so that neither tuning nor a resonating capacitor is necessary. Experimental measurements show that the system draws power from 30-mV signals when k C is 0.0046 and coil separation is 11.35 mm, and this threshold voltage only changes 13.6 mV across 100-150 kHz, which is a 27.1% lower threshold voltage that is 36 × less sensitive than its resonating counterpart. The peak efficiency of the receiver when rectifying to 1.2 V is 82% at 224 μW and 125 kHz and average efficiency is 76% for 90-386-mV coil voltages.
doi_str_mv 10.1109/JSSC.2013.2280053
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Experimental measurements show that the system draws power from 30-mV signals when k C is 0.0046 and coil separation is 11.35 mm, and this threshold voltage only changes 13.6 mV across 100-150 kHz, which is a 27.1% lower threshold voltage that is 36 × less sensitive than its resonating counterpart. The peak efficiency of the receiver when rectifying to 1.2 V is 82% at 224 μW and 125 kHz and average efficiency is 76% for 90-386-mV coil voltages.</description><identifier>ISSN: 0018-9200</identifier><identifier>EISSN: 1558-173X</identifier><identifier>DOI: 10.1109/JSSC.2013.2280053</identifier><identifier>CODEN: IJSCBC</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Applied sciences ; Batteries ; Capacitors ; Coils ; Contactless charging ; Design. Technologies. Operation analysis. Testing ; Dielectric, amorphous and glass solid devices ; Diodes ; Electronic equipment and fabrication. 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Passive components, printed wiring boards, connectics</subject><subject>Electronics</subject><subject>Exact sciences and technology</subject><subject>inductive power transmission</subject><subject>inductively coupling</subject><subject>Integrated circuits</subject><subject>Logic gates</subject><subject>low-threshold rectifier</subject><subject>Magnetic resonance</subject><subject>Receivers</subject><subject>Semiconductor electronics. Microelectronics. Optoelectronics. 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Periodically coupling power wirelessly is one way of replenishing onboard batteries, except that small receiver coils suffer from low coupling factors k C and induce low electromotive-force voltages. Today, receivers store and resonate incoming energy between the receiving coil and an off-chip capacitor until the voltage rises sufficiently high for a diode-bridge rectifier to steer power into a battery. The capacitor, however, requires board space and constrains the source to a particular frequency. The 180-nm CMOS power receiver presented in this paper removes the diode bridge, which establishes a minimum voltage below which the system cannot derive power, so that neither tuning nor a resonating capacitor is necessary. Experimental measurements show that the system draws power from 30-mV signals when k C is 0.0046 and coil separation is 11.35 mm, and this threshold voltage only changes 13.6 mV across 100-150 kHz, which is a 27.1% lower threshold voltage that is 36 × less sensitive than its resonating counterpart. The peak efficiency of the receiver when rectifying to 1.2 V is 82% at 224 μW and 125 kHz and average efficiency is 76% for 90-386-mV coil voltages.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/JSSC.2013.2280053</doi><tpages>11</tpages></addata></record>
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source IEEE Electronic Library (IEL)
subjects Applied sciences
Batteries
Capacitors
Coils
Contactless charging
Design. Technologies. Operation analysis. Testing
Dielectric, amorphous and glass solid devices
Diodes
Electronic equipment and fabrication. Passive components, printed wiring boards, connectics
Electronics
Exact sciences and technology
inductive power transmission
inductively coupling
Integrated circuits
Logic gates
low-threshold rectifier
Magnetic resonance
Receivers
Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices
Switches
wireless power transfer
title 180-nm CMOS Wideband Capacitor-Free Inductively Coupled Power Receiver and Charger
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