Wireless Energy Transfer by Resonant Inductive Coupling
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Coupled Resonator Based Wireless Power Transfer for Bioelectronics Henry Mei Purdue University
Purdue University Purdue e-Pubs Open Access Dissertations Theses and Dissertations 4-2016 Coupled resonator based wireless power transfer for bioelectronics Henry Mei Purdue University Follow this and additional works at: https://docs.lib.purdue.edu/open_access_dissertations Part of the Biomedical Engineering and Bioengineering Commons, and the Electromagnetics and Photonics Commons Recommended Citation Mei, Henry, "Coupled resonator based wireless power transfer for bioelectronics" (2016). Open Access Dissertations. 678. https://docs.lib.purdue.edu/open_access_dissertations/678 This document has been made available through Purdue e-Pubs, a service of the Purdue University Libraries. Please contact [email protected] for additional information. Graduate School Form 30 Updated ¡ ¢¡£ ¢¡¤ ¥ ¦§¨©§ § ¨ ¨ ©§ © !!" ! #$%& %& '( )*+'%,- '$.' ' $ * ' $*&% &/0%&&*+'.'%( 1 2 +*2. +*0 - 3 41'%'5*0 w w (+ '$* 0* +**(, 6 7 &.22+( *0 -'$*,%1.5 * . %1%1 )( %'' ** 8 9 : ; < 7 << = ¡¢£¤¥ ¦§¨ ©ª « ¬ ¥ ¥ ¥ ® ¬¯ ¬° ¥ ± ² ¢ >? @ABCBD@?EFGHI?JKBLMBNILNDOILBPD@?? L CG @ ABD@OLBI @ QI@AB>ABDQDRS QDDBP@N@Q?I TMPBBFBI@U V OCKQWN@ Q?I SB KNGUNILXBP @ QEQWN @ Q ?ISQDWKNQFBP YZPN L ON @B [ WA??K \ ?PF ]^_U @AQD@ABDQDRLQDDBP @N@Q?INLABPBD @ ? @AB`P?aQDQ?ID ? E V OPLOBbIQaBP D Q@GcD dV?KQWG ?E e f g h I@BMPQ@G QI BDBNPWA NI L @ ABODB?EW?`GPQMA@FN@ B P QNK ¡¢£ ¤¥ i22 +( *0 -j.k (+ l +(, *&&(+m&n 9 : = ¬ ³ ´µ¶ ·¢ ¸¹ º¹»¼½¾ i22 +( *0 - 9 : = opqrstuvpwpxqyuzp{uq|}yqr ~ qup ysyqz wqup i COUPLED RESONATOR BASED WIRELESS POWER TRANSFER FOR BIOELECTRONICS A Dissertation Submitted to the Faculty of Purdue University by Henry Mei In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy May 2016 Purdue University West Lafayette, Indiana ii I dedicate this dissertation to my wife, Jocelyne, who has provided her undying love and unwavering support from which this most selfish endeavor would never have ¡¢£¤¥¦§¨©¥ been possible. -
Active Balun with Center-Tapped Inductor and Double-Balanced Gilbert Mixer for GNSS Applications
electronics Article Active Balun with Center-Tapped Inductor and Double-Balanced Gilbert Mixer for GNSS Applications Daniel Pietron 1,* , Tomasz Borejko 1,2 and Witold Adam Pleskacz 1 1 Institute of Microelectronics & Optoelectronics, Warsaw University of Technology, ul. Koszykowa 75, 00-662 Warsaw, Poland; [email protected] or [email protected] (T.B.); [email protected] (W.A.P.) 2 ChipCraft Sp. z o.o., ul. Dobrza´nskiego3, lok. BS073, 20-262 Lublin, Poland * Correspondence: [email protected] Abstract: A new 1.575 GHz active balun with a classic double-balanced Gilbert mixer for global navigation satellite systems is proposed herein. A simple, low-noise amplifier architecture is used with a center-tapped inductor to generate a differential signal equal in amplitude and shifted in phase by 180◦. The main advantage of the proposed circuit is that the phase shift between the outputs is always equal to 180◦, with an accuracy of ±5◦, and the gain difference between the balun outputs does not change by more than 1.5 dB. This phase shift and gain difference between the outputs are also preserved for all process corners, as well as temperature and voltage supply variations. In the balun design, a band calibration system based on a switchable capacitor bank is proposed. The balun and mixer were designed with a 110 nm CMOS process, consuming only a 2.24 mA current from a 1.5 V supply. The measured noise figure and conversion gain of the balun and mixer were, respectively, NF = 7.7 dB and GC = 25.8 dB in the band of interest. -
Up-And-Coming Physical Concepts of Wireless Power Transfer
Up-And-Coming Physical Concepts of Wireless Power Transfer Mingzhao Song1,2 *, Prasad Jayathurathnage3, Esmaeel Zanganeh1, Mariia Krasikova1, Pavel Smirnov1, Pavel Belov1, Polina Kapitanova1, Constantin Simovski1,3, Sergei Tretyakov3, and Alex Krasnok4 * 1School of Physics and Engineering, ITMO University, 197101, Saint Petersburg, Russia 2College of Information and Communication Engineering, Harbin Engineering University, 150001 Harbin, China 3Department of Electronics and Nanoengineering, Aalto University, P.O. Box 15500, FI-00076 Aalto, Finland 4Photonics Initiative, Advanced Science Research Center, City University of New York, NY 10031, USA *e-mail: [email protected], [email protected] Abstract The rapid development of chargeable devices has caused a great deal of interest in efficient and stable wireless power transfer (WPT) solutions. Most conventional WPT technologies exploit outdated electromagnetic field control methods proposed in the 20th century, wherein some essential parameters are sacrificed in favour of the other ones (efficiency vs. stability), making available WPT systems far from the optimal ones. Over the last few years, the development of novel approaches to electromagnetic field manipulation has enabled many up-and-coming technologies holding great promises for advanced WPT. Examples include coherent perfect absorption, exceptional points in non-Hermitian systems, non-radiating states and anapoles, advanced artificial materials and metastructures. This work overviews the recent achievements in novel physical effects and materials for advanced WPT. We provide a consistent analysis of existing technologies, their pros and cons, and attempt to envision possible perspectives. 1 Wireless power transfer (WPT), i.e., the transmission of electromagnetic energy without physical connectors such as wires or waveguides, is a rapidly developing technology increasingly being introduced into modern life, motivated by the exponential growth in demand for fast and efficient wireless charging of battery-powered devices. -
Double-Loop Coil Design for Wireless Power Transfer to Embedded Sensors on Spindles
602 Journal of Power Electronics, Vol. 19, No. 2, pp. 602-611, March 2019 https://doi.org/10.6113/JPE.2019.19.2.602 JPE 19-2-25 ISSN(Print): 1598-2092 / ISSN(Online): 2093-4718 Double-Loop Coil Design for Wireless Power Transfer to Embedded Sensors on Spindles Suiyu Chen*, Yongmin Yang†, and Yanting Luo* †,*Science and Technology on Integrated Logistics Support Laboratory, National University of Defense Technology, Changsha, China Abstract The major drawbacks of magnetic resonant coupled wireless power transfer (WPT) to the embedded sensors on spindles are transmission instability and low efficiency of the transmission. This paper proposes a novel double-loop coil design for wirelessly charging embedded sensors. Theoretical and finite-element analyses show that the proposed coil has good transmission performance. In addition, the power transmission capability of the double-loop coil can be improved by reducing the radius difference and width difference of the transmitter and receiver. It has been demonstrated by analysis and practical experiments that a magnetic resonant coupled WPT system using the double-loop coil can provide a stable and efficient power transmission to embedded sensors. Key words: Embedded sensors, Magnetic resonant coupled, Spindle, WPT I. INTRODUCTION inductive coupled WPT systems is greatly affected by the angular and axial misalignments between the transmitter and Almost all modern electromechanical systems are driven by receiver. In addition, its transmission distance is limited to a few spindles. Thus, it is necessary to monitor the running status of centimeters [6]-[10]. When compared to inductive coupling spindles to ensure the reliability and security of these systems WPT systems, magnetic resonant coupled WPT systems can [1]. -
Wireless Power Transmission
International Journal of Scientific & Engineering Research, Volume 5, Issue 10, October-2014 125 ISSN 2229-5518 Wireless Power Transmission Mystica Augustine Michael Duke Final year student, Mechanical Engineering, CEG, Anna university, Chennai, Tamilnadu, India [email protected] ABSTRACT- The technology for wireless power transfer (WPT) is a varied and a complex process. The demand for electricity is much higher than the amount being produced. Generally, the power generated is transmitted through wires. To reduce transmission and distribution losses, researchers have drifted towards wireless energy transmission. The present paper discusses about the history, evolution, types, research and advantages of wireless power transmission. There are separate methods proposed for shorter and longer distance power transmission; Inductive coupling, Resonant inductive coupling and air ionization for short distances; Microwave and Laser transmission for longer distances. The pioneer of the field, Tesla attempted to create a powerful, wireless electric transmitter more than a century ago which has now seen an exponential growth. This paper as a whole illuminates all the efficient methods proposed for transmitting power without wires. —————————— —————————— INTRODUCTION Wireless power transfer involves the transmission of power from a power source to an electrical load without connectors, across an air gap. The basis of a wireless power system involves essentially two coils – a transmitter and receiver coil. The transmitter coil is energized by alternating current to generate a magnetic field, which in turn induces a current in the receiver coil (Ref 1). The basics of wireless power transfer involves the inductive transmission of energy from a transmitter to a receiver via an oscillating magnetic field. -
Crystal Radio Set Systems: Design, Measurement, and Improvement Volume II a Web Book by Ben Tongue
Crystal Radio Set Systems: Design, Measurement, and Improvement Volume II A web book by Ben Tongue First published: 10 Jul 1999; Revised: 01/06/10 i NOTES: ii 185 PREFACE Note: An easy way to use a DVM ohmmeter to check if a ferrite is made of MnZn of NiZn material is to place the leads of the ohmmeter on a bare part of the test ferrite and read the The main purpose of these Articles is to show how resistance. The resistance of NiZn will be so high that the Engineering Principles may be applied to the design of crystal ohmmeter will show an open circuit. If the ferrite is of the radios. Measurement techniques and actual measurements are MnZn type, the ohmmeter will show a reading. The reading described. They relate to selectivity, sensitivity, inductor (coil) was about 100k ohms on the ferrite rods used here. and capacitor Q (quality factor), impedance matching, the diode SPICE parameters saturation current and ideality factor, #29 Published: 10/07/2006; Revised: 01/07/08 audio transformer characteristics, earphone and antenna to ground system parameters. The design of some crystal radios that embody these principles are shown, along with performance measurements. Some original technical concepts such as the linear-to-square-law crossover point of a diode detector, contra-wound inductors and the 'benny' are presented. Please note: If any terms or concepts used here are unclear or obscure, please check out Article # 00 for possible explanations. If there still is a problem, e-mail me and I'll try to assist (Use the link below to the Front Page for my Email address). -
Optimization of Low Frequency Litz-Wire RF Coils
Optimization of Low Frequency Litz-wire RF Coils J.A. Croon, II. M. fkJrSbooll1, A. F. Mehlkopf Fi7culty of Applied Physics, DeFt IJniversity of Technology, P.O. Box 5046, 2600 GA Delft, 77zeNetherlands INTRODUCTION Equations ]4] and [5] show that the skin losses are proportional to the In MRI the patient or sample losses increase with the square of the resistivity while the proximity losses are proportional to the conductiv- resonance frequency. This makes coil losses significant at low field ity. The rota1 losses are minimized if the derivative of P,,,, to p is zero. strengths. dP,oss %kin Rprox_ It is well known (1) that for frequencies of several hundreds of l&z - =--- - 0 or Rski,, = R WI stranded or litz wires can have lower losses than conventional wires, do P P PYqX Here we will investigate and present the optimization of copper solenoid coils for room temperature and for liquid nitrogen temperature. Thus the maximum coil quality is achieved if the skin losses equal the For litz wire coils we distinguish three types of losses: proximity losses. 1. losses within each considered strand, 2. proximity losses in the surrounding strands and RESULTS 3. eddy losses the environment of the coil (mainly determined by the The results of table 1 concern solenoids with a single litz wire and with sample losses). The losses within the considered strands are called skin six parallel litz wires. The six parallel wires are placed above each losses. We will show that the maximum coil quality is achieved if the other and twisted such that the losses in each parallel wire are the skin losses are equal to the proximity losses. -
A Critical Review of Wireless Power Transfer Via Strongly Coupled Magnetic Resonances
Energies 2014, 7, 4316-4341; doi:10.3390/en7074316 OPEN ACCESS energies ISSN 1996-1073 www.mdpi.com/journal/energies Review A Critical Review of Wireless Power Transfer via Strongly Coupled Magnetic Resonances Xuezhe Wei 1,2,*, Zhenshi Wang 1,2 and Haifeng Dai 1,2 1 Clean Energy Automotive Engineering Center, Tongji University, Shanghai 201804, China; E-Mails: [email protected] (Z.W.); [email protected] (H.D.) 2 College of Automotive Studies, Tongji University, Shanghai 201804, China * Author to whom correspondence should be addressed; E-Mail: [email protected]; Tel.: +86-21-6958-3764; Fax: +86-21-6958-9121. Received: 21 March 2014; in revised form: 9 May 2014 / Accepted: 30 June 2014 / Published: 7 July 2014 Abstract: Strongly coupled magnetic resonance (SCMR), proposed by researchers at MIT in 2007, attracted the world’s attention by virtue of its mid-range, non-radiative and high-efficiency power transfer. In this paper, current developments and research progress in the SCMR area are presented. Advantages of SCMR are analyzed by comparing it with the other wireless power transfer (WPT) technologies, and different analytic principles of SCMR are elaborated in depth and further compared. The hot research spots, including system architectures, frequency splitting phenomena, impedance matching and optimization designs are classified and elaborated. Finally, current research directions and development trends of SCMR are discussed. Keywords: wireless power transfer; strongly coupled magnetic resonances; mid-range non-radiative high-efficient power transfer 1. Introduction Wireless power transfer is not strange to human beings, since as early as 1889 Nikola Tesla had invented the famous Tesla coils which can transfer power wirelessly. -
Figure 1 Old Huge Magnetic Receiving Loop Antennas
ANTENTOP- 02- 2004, # 006 Old Receiving Magnetic Loop Antennas Igor Grigorov, RK3ZK [email protected] Receiving magnetic loop antennas were widely used in the professional radio communication from the beginning of the 20 Century. Since 1906 magnetic loop antennas were used for direction finding purposes needed for navigation of ships and planes. Later, from 20s, magnetic loop antennas were used for broadcasting reception. In the USSR in 20- 40 years of the 20 Century when broadcasting was gone on LW and MW, huge loop antennas were used on Reception Broadcasting Centers (see pages 93- 94 about USSRs RBC). Magnetic loop antennas worldwide were used for reception service radio stations working in VLW, LW and MW. The article writes up several designs of such old receiving loop antennas. LW- MW Huge Receiving Loop Fig. 2 shows a typical connection of the above mention Antennas for Broadcasting and huge magnetic receiving loop antennas designed for Direction Finding working on one fixing frequency to the receiver. To a resonance the loop A1 is tuned by lengthening coil L1 In old radio textbooks you can find description of old (sometimes two lengthening coils switched symmetrically magnetic receiving loop antennas. As a rule, old to both side of the loop were used) and variable air- magnetic receiving loop antennas had a triangle or dielectric capacitor C1. T1 did connection with antenna square shape, a side of the triangle or square had feedline. L1, C1 and T1, as a rule, are placed directly length in 10-20 meters. The huge square was put near the antenna keeping minimum length for wires from on to a corner. -
A Novel Single-Wire Power Transfer Method for Wireless Sensor Networks
energies Article A Novel Single-Wire Power Transfer Method for Wireless Sensor Networks Yang Li, Rui Wang * , Yu-Jie Zhai , Yao Li, Xin Ni, Jingnan Ma and Jiaming Liu Tianjin Key Laboratory of Advanced Electrical Engineering and Energy Technology, Tiangong University, Tianjin 300387, China; [email protected] (Y.L.); [email protected] (Y.-J.Z.); [email protected] (Y.L.); [email protected] (X.N.); [email protected] (J.M.); [email protected] (J.L.) * Correspondence: [email protected]; Tel.: +86-152-0222-1822 Received: 8 September 2020; Accepted: 1 October 2020; Published: 5 October 2020 Abstract: Wireless sensor networks (WSNs) have broad application prospects due to having the characteristics of low power, low cost, wide distribution and self-organization. At present, most the WSNs are battery powered, but batteries must be changed frequently in this method. If the changes are not on time, the energy of sensors will be insufficient, leading to node faults or even networks interruptions. In order to solve the problem of poor power supply reliability in WSNs, a novel power supply method, the single-wire power transfer method, is utilized in this paper. This method uses only one wire to connect source and load. According to the characteristics of WSNs, a single-wire power transfer system for WSNs was designed. The characteristics of directivity and multi-loads were analyzed by simulations and experiments to verify the feasibility of this method. The results show that the total efficiency of the multi-load system can reach more than 70% and there is no directivity. Additionally, the efficiencies are higher than wireless power transfer (WPT) systems under the same conductions. -
Experiment of Magnetic Resonant Coupling Three-Phase Wireless Power Transfer Phase Wireless Power Transfer
Experiment of Magnetic Resonant Coupling ThreeThree----phasephase Wireless Power Transfer Yusuke Tanikawa, Masaki Kato, Takehiro Imura, Yoichi Hori Organized by Hosted by In collaboration with Supported by 2/26 What is our research? Organized by Hosted by In collaboration with Supported by 3/26 Contents 0. What is our study? : Movie 1. Background of Wireless Power Transfer 1.1. General information of WPT 1.2. Why three phase? 2. Approach of our study 2.1. General info. & parameters 2.2. Theoretical formula 2.3. Experiment and result 3. Conclusion and future works Organized by Hosted by In collaboration with Supported by 4/26 Contents 0. What is our study? : Movie 1. Background of Wireless Power Transfer 1.1. General information of WPT 1.2. Why three phase? 2. Approach of our study 2.1. General info. & parameters 2.2. Theoretical formula 2.3. Experiment and result 3. Conclusion and future works Organized by Hosted by In collaboration with Supported by 5/26 1.1. General info. for WPT 1/3 Wireless Power Transfer (WPT) Applications: EV , mobile, and battery charger Conventional WPT: Single phase AC transfer Organized by Hosted by In collaboration with Supported by 6/26 1.1. General info. for WPT 2/3 Three methods of WPT technologies Magnetic Magnetic Resonant Methods Microwave Induction Coupling Images Transfer Gap Up to 0.2 m Up to 10 m A few hundred km Efficiency Up to 95% Up to 97% Up to 60 % Robustness for Poor Great Good Displacement Organized by Hosted by In collaboration with Supported by 6/26 7/26 1.1. -
Novel Implementations of Wideband Tightly Coupled Dipole Arrays for Wide-Angle Scanning
Novel Implementations of Wideband Tightly Coupled Dipole Arrays for Wide-Angle Scanning Dissertation Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Ersin Yetisir, B.S., M.S. Graduate Program in Electrical and Computer Engineering The Ohio State University 2015 Dissertation Committee: John L. Volakis, Advisor Nima Ghalichechian, Co-advisor Chi-Chih Chen Fernando L. Teixeira © Copyright by Ersin Yetisir 2015 Abstract Ultra-wideband (UWB) antennas and arrays are essential for high data rate communications and for addressing spectrum congestion. Tightly coupled dipole arrays (TCDAs) are of particular interest due to their low-profile, bandwidth and scanning range. But existing UWB (>3:1 bandwidth) arrays still suffer from limited scanning, particularly at angles beyond 45° from broadside. Almost all previous wideband TCDAs have employed dielectric layers above the antenna aperture to improve scanning while maintaining impedance bandwidth. But even so, these UWB arrays have been limited to no more than 60° away from broadside. In this work, we propose to replace the dielectric superstrate with frequency selective surfaces (FSS). In effect, the FSS is used to create an effective dielectric layer placed over the antenna array. FSS also enables anisotropic responses and more design freedom than conventional isotropic dielectric substrates. Another important aspect of the FSS is its ease of fabrication and low weight, both critical for mobile platforms (e.g. unmanned air vehicles), especially at lower microwave frequencies. Specifically, it can be fabricated using standard printed circuit technology and integrated on a single board with active radiating elements and feed lines.