Resonant Inductive Coupling Wireless Power Transfer



Similar documents
Nanonetworks: a novel communication paradigm

An equivalent circuit of a loop antenna.

Fundamentals of radio communication

Impedance Matching and Matching Networks. Valentin Todorow, December, 2009

ANALYSIS AND VERIFICATION OF A PROPOSED ANTENNA DESIGN FOR AN IMPLANTABLE. RFID TAG AT 915 MHz RAHUL BAKORE

Tesla Wireless Energy Transfer at CCC

RFID Receiver Antenna Project for Mhz Band

Understanding SMD Power Inductors. Application Note. July 2011

HIGHLY RESONANT WIRELESS POWER TRANSFER IN SUBSEA APPLICATIONS

Wireless Power Transfer System Design. Julius Saitz ANSYS

EM Noise Mitigation in Circuit Boards and Cavities

Single Transistor FM Transmitter Design

The performance improvement by ferrite loading means - increasing, - increasing of ratio, implicitly related to the input impedance.

Wireless Power for Remote Monitoring Applications

EMC Standards: Standards of good EMC engineering

POLITECNICO DI MILANO PhD School Doctoral Program in Electrical Engineering Cycle XXIV

National Laboratory of Antennas and Microwave Technology Xidian University Xi an, Shaanxi , China

Efficient Meshing in Sonnet

Analysis of Broadband Slot Cut Semi-Circular Microstrip Antennas

Exposure Assessment of a High-Resonance Wireless Power Transfer System under the Misaligned Condition

Energy Harvesting in Practical Applications. Roy Freeland President, Perpetuum Ltd

Simulation of Mobile Phone Antenna Performance

Lecture 24. Inductance and Switching Power Supplies (how your solar charger voltage converter works)

AN2866 Application note

Co-simulation of Microwave Networks. Sanghoon Shin, Ph.D. RS Microwave

Radiated Emission and Susceptibility

EMC Countermeasures for In-Vehicle Communication Networks

Design of 2D waveguide networks for the study of fundamental properties of Quantum Graphs

Comparison of Power Título Transmission Line Models with Finite Elements

Inductive Charging Technique

2.996/6.971 Biomedical Devices Design Laboratory Lecture 2: Fundamentals and PCB Layout

ENERGY HARVESTING FROM RF SIGNAL

Transmission Line Transformers

RF energy harvester based on MEMS

Basic Wire Antennas. Part II: Loops and Verticals

1. INTRODUCTION. There are different frequency bans according to the range of frequencies shown: 1.1 Electromagnetic Spectrum

Software for Design NMR Probes Using the Shielded Split Ring and the Shielded Symmetrical Band Resonators

Antenna A mean for radiating and receiving radio waves Transitional structure between free-space and a guiding device. Application: Radiation

Connectivity in a Wireless World. Cables Connectors A Special Supplement to

Design of an U-slot Folded Shorted Patch Antenna for RF Energy Harvesting

a leap ahead in analog

Wireless RF Distribution in Buildings using Heating and Ventilation Ducts

Since any real component also has loss due to the resistive component, the average power dissipated is 2 2R

Time and Frequency Domain Analysis for Right Angle Corners on Printed Circuit Board Traces

Flexible PCB Antenna with Cable Integration Application Note Version 2

2/20/ Transmission Lines and Waveguides.doc 1/3. and Waveguides. Transmission Line A two conductor structure that can support a TEM wave.

A wave lab inside a coaxial cable

Energy Harvesting Powered Wireless Sensor Node and Asset Tracking Solutions in Random Vibration Environments

How To Understand The Power Of An Freddi Tag (Rfid) System

Experiment 8: Undriven & Driven RLC Circuits

IFI5481: RF Circuits, Theory and Design

CITY UNIVERSITY OF HONG KONG. A Study of Electromagnetic Radiation and Specific Absorption Rate of Mobile Phones with Fractional Human Head Models

LVDS Technology Solves Typical EMI Problems Associated with Cell Phone Cameras and Displays

Nano Stepping Notch Filter Jim Hagerman

Today s handsets have to meet tough ELECTROMAGNETIC SIMULATION OF MOBILE PHONE ANTENNA PERFORMANCE

Selecting Receiving Antennas for Radio Tracking

EMC STANDARDS STANDARDS AND STANDARD MAKING BODIES. International. International Electrotechnical Commission (IEC)

Application Note. So You Need to Measure Some Inductors?

Design Challenges for PoDL Coupling Circuit in 100BASE-T1 and 1000BASE-T1

Circuits with inductors and alternating currents. Chapter 20 #45, 46, 47, 49

An octave bandwidth dipole antenna

12. The current in an inductor is changing at the rate of 100 A/s, and the inductor emf is 40 V. What is its self-inductance?

CONCEPT-II. Overview of demo examples

Pre-Compliance Test Method for Radiated Emissions of Automotive Components Using Scattering Parameter Transfer Functions

Micro Power Generators. Sung Park Kelvin Yuk ECS 203

Insight on mobile phones and communication system:

Eatman Associates 2014 Rockwall TX rev. October 1, Striplines and Microstrips (PCB Transmission Lines)

RigExpert AA-30 Antenna Analyzer (0.1 to 30 MHz) AA-54 Antenna Analyzer (0.1 to 54 MHz) User s manual

Chinese Academy of Sciences, 865 Chang Ning Road, Shanghai , China

ISPS2014 Workshop Energy to Smart Grids Presenting results of ENIAC project: E2SG (Energy to Smart Grid)

VBA Macro for construction of an EM 3D model of a tyre and part of the vehicle

Mitigating Power Bus Noise with Embedded Capacitance in PCB Designs

Eðlisfræði 2, vor 2007

Minimizing crosstalk in a high-speed cable-connector assembly.

Edmund Li. Where is defined as the mutual inductance between and and has the SI units of Henries (H).

Effects of Mobile Phone Radiation onto Human Head with Variation of Holding Cheek and Tilt Positions

Human Exposure Limits

Application Note: PCB Design By: Wei-Lung Ho

Design and Electromagnetic Modeling of E-Plane Sectoral Horn Antenna For Ultra Wide Band Applications On WR-137 & WR- 62 Waveguides

AVR2006: Design and characterization of the Radio Controller Board's 2.4GHz PCB Antenna. Application Note. Features.

RLC Resonant Circuits

Design & Simulation of 8-Shape Slotted Microstrip Patch Antenna

Understanding the Electrical Performance of Category Cables

Demystifying Wireless for Real-World Measurement Applications

DRAFT. University of Pennsylvania Moore School of Electrical Engineering ESE319 Electronic Circuits - Modeling and Measurement Techniques

J. Zhang, J.-Z. Gu, B. Cui, andx. W. Sun Shanghai Institute of Microsystem & Information Technology CAS Shanghai , China


Human Exposure to Outdoor PLC System

READER COMPONENTS. mifare (14443A) MHz RFID Proximity Antennas. November Revision 1.0 PUBLIC. Philips Semiconductors

INTERNET OF THINGS 1

Signal Integrity: Tips and Tricks

SIW 2D PLANAR ARRAY WITH FOUR CROSS SLOTS RADIATOR AND TUNING VIAS

Effects of Cell Phone Radiation on the Head. BEE 4530 Computer-Aided Engineering: Applications to Biomedical Processes

Electronic filters design tutorial -2

Design Considerations for RF Energy Harvesting Devices

Design Optimization of Printed Circuit Board Embedded Inductors through Genetic Algorithms with Verification by COMSOL

Transcription:

NaNoNetworking Summit 2012: RIC Wireless Power Transfer June 22nd 2012, N3CAT UPC Resonant Inductive Coupling Wireless Power Transfer Elisenda Bou Balust

Outline Introduction Energy Challenges in Nanotechnology Resonant Inductive Coupling RIC Scalability WPT Based Active Energy Harvesting New Nano Applications Wireless Nano Sensor Networks Claytronics Nano materials

Energy Challenges in Nanotechnology Enabled Wireless Comm. WNSN All nodes need to be individually powered Ambient Energy is not enough Claytronics ACTIVE energy harvesting Resonant Inductive Coupling Graphene Inductors

Introduction Overview Resonant Inductive Coupling is a type of Electromagnetic WPT Very promising efficiencies Above 80% PTEff. Relative large distances 3 times the tx/rx diameters. Potential applications Electric vehicle charging Sensor networks Biomedical Implants Commercial electronic devices RIC is a very novel technology (< 4y)

Introduction Radiative & Non Radiative behaviors Electromagnetic WPT is the transmission of EM fields Dual composition of EM fields a WPT system can behave differently depending on the separation between Tx and Rx Non Radiative (Near Field Region) changes in current/charge distrib. Radiative (Far Field Region) changes in Magnetic/Electric fields. Where is the limit? Maxwell's equations for an Infinitesimal Dipole Quasi stationary term Radiative term Induction term

Introduction Radiative & Non Radiative behaviors The region where all the contributions are equal is the boundary region between near and far field. Separation not sharp mid range zone where radiative and nonradiative fields coexist. If r << λ/2π Electrostatic & induction terms non radiative (reactive) near field zone If λ/2π < r < λ Induction & Radiation terms mid range If r >> λ/2π Radiation term dominates far field zone

Introduction EM. Inductive WPT First demonstrated in the early 20th century by Nikola Tesla, but thought impractical due to the undesirably large electric fields. In 1960 WPT EMI was reintroduced for biomedical applications (artificial hearts). Since then, commonly used in implantable devices. These inductors, such as typical transformers, required a very short distance between transmitter and receiver (centimeters range).

Introduction Radiative & Non Radiative behaviors Later systems implemented resonant transmitter coils Each coil capacitively loaded forming a tuned LC resonating circuit at a common frequency. Inductive links used in medical and consumer applications, but limited to the near range (less than the dimensions of the coils). Resonant Non Resonant

Introduction Radiative & Non Radiative behaviors In 2007, EMI links extended to larger ranges (several times the diameter of the antennas) stretching RIC in strong coupling regime. Demonstrated lighting a bulb at 2m with 40% Efficiency Strong coupled RIC attracted lot of attention Harmless to humans (non radiative). No direct line of sight needed Good efficiencies at several meters. RIC is foreseen as a key enabling technology for wireless power transfer in the following years.

Introduction Radiative & Non Radiative behaviors

Exploring RIC Scalability There are scattered examples of RIC for different frequencies/sizes of the coils

Exploring RIC Scalability RIC efficiency as a function up to 10 times the radii of the antennas.

WPT Based Active Energy Harvesting EH would allow successful deployment of battery less self powered Wireless sensor networks (WSN) nodes, biomedical implants and body area networks Despise EH is already successful in niche applications, the most ubiquitous source of energy, EM harvesting, is still not feasible. To circumvent the current short and mid terms limits of EH technologies artificially increase ambient energy active radiation of a single energy source (energy broadcast). The high efficiency WPT RIC systems become of strong interest as an enabler of active electromagnetic WPT based energy harvesting.

Nano Materials: Graphene Based coils How to increase the range of the system? Decrease losses (improve Q) To reduce losses, several technologies have been proposed: Superconducting dielectric less coils ohmic losses negligible More complexity Litz Wire Coils minimize skin & proximity effects Low frequencies 1 2MHz. Because high frequency/low loss coils are necessary in Wireless Power and Data Systems, we propose to use new materials such as graphenebased nano coils for the design and implementation of active energy harvesting systems.

Nano Materials: Graphene Based coils High Frequency Behavior of Graphene Based Interconnects Part II: Impedance Analysis and Implications for Inductor Design Deblina Sarkar, Student Member, IEEE, Chuan Xu, Student Member, IEEE, Hong Li, Student Member, IEEE, and Kaustav Banerjee, Senior Member, IEEE Diameter = 200 μm, N=4, Wire width= 8 μm, Wire thickness H = 2 μm

Nano Materials: Graphene Based coils Same graphene doped coils simulated with Finite Element Field Solver FEKO Differences with previous results due to the non ideal dielectric substrate used.

Wireless Nano Sensor Networks One of the potential applications of RIC systems is WPT networks. Due to the behavior of RIC systems, this WPT method is very suitable for broadcast applications where coils could be active (resonant) or inactive (non resonating) without inquiring in significant losses to the transmitter's power. Because in RIC systems, antennas act as transmitter and receiver at the same time, WPT meshed networks could be implemented and miniaturized.

Wireless Nano Sensor Networks RIC inductors can operate as transmitter and receiver at the same time Increase in distance range by using the different nodes as repeaters.

Claytronics Inteligent Matter RIC can be used as a potential means for providing power to catoms without using electrical connections. WPT to multiple small receivers has been demonstrated by Prof. Goldstein. Magnetic Resonant Coupling As a Potential Means for Wireless Power Transfer to Multiple Small Receivers Benjamin L. Cannon, James F. Hoburg, Daniel D. Stancil and Seth Copen Goldstein

Conclusions In WNSN and claytronics, every node needs to be powered individually. The challenge to power this nodes using energy harvesting is still unsolved. We propose to use Active Energy Harvesting to circumvent the energy requirements. Because of its scalability in frequency and size, Resonant Inductive Coupling is proposed as a method to perform Active Energy Harvesting in the nano scale. Graphene based inductor antennas have been simulated to act as the transmitters and receivers of such a RIC system.