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首页> 外文期刊>IEEE Journal of Solid-State Circuits >180-nm CMOS Wideband Capacitor-Free Inductively Coupled Power Receiver and Charger
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180-nm CMOS Wideband Capacitor-Free Inductively Coupled Power Receiver and Charger

机译:180 nm CMOS宽带无电容电感耦合功率接收器和充电器

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摘要

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 ${rm k}_{rm C}$ 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 ${rm k}_{rm C}$ 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$times$ less sensitive than its resonating counterpart. The peak efficiency of the receiver when rectifying to 1.2 V is 82% at 224 $muhbox{W}$ and 125 kHz and average efficiency is 76% for 90–386-mV coil voltages.
机译:诸如生物医学植入物和嵌入式传感器之类的无线微系统是从微小的封装内源中获取能量的,不幸的是,这些源很容易耗尽,这意味着使用寿命很短。无线地周期性地耦合功率是补充车载电池的一种方法,除了较小的接收器线圈具有低耦合因子$ {rm k} _ {rm C} $并产生低电动势电压之外。如今,接收器在接收线圈和片外电容器之间存储并谐振输入的能量,直到电压升高到足以使二极管桥式整流器将功率引到电池中为止。然而,电容器需要占用电路板空间,并将电源限制在特定的频率。本文介绍的180nm CMOS电源接收器去除了二极管电桥,二极管电桥建立了一个最小电压,低于该电压系统将无法获得功率,因此无需调谐或谐振电容器。实验测量表明,当$ {rm k} _ {rm C} $为0.0046且线圈间距为11.35 mm时,系统从30 mV信号中汲取功率,并且此阈值电压在100–150 kHz范围内仅变化13.6 mV,即阈值电压降低了27.1%,其灵敏度比谐振电压低36倍。整流至1.2 V时,接收器的峰值效率在224 $ muhbox {W} $和125 kHz时为82%,而在90-386 mV线圈电压下的平均效率为76%。

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