Time Reversed Electromagnetic Wave Propagation as a Novel Method of Wireless Power Transfer

Similar documents
Inducing Chaos in the p/n Junction

Chaos Experiments. Steven M. Anlage Renato Mariz de Moraes Tom Antonsen Ed Ott. Physics Department University of Maryland, College Park

Delayed Feedback and GHz-Scale Chaos on the Driven Diode-Terminated Transmission Line

RF Upset and Chaos in Circuits: Basic Investigations. Steven M. Anlage, Vassili Demergis, Ed Ott, Tom Antonsen

LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION. Instructor: Kazumi Tolich

Novel Features of Computational EM and Particle-in-Cell Simulations. Shahid Ahmed. Illinois Institute of Technology

Is Quantum Mechanics Chaotic? Steven Anlage

LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION. Instructor: Kazumi Tolich

Ruby crystals and the first laser A spectroscopy experiment

Technique for the electric and magnetic parameter measurement of powdered materials

Production of X-rays. Radiation Safety Training for Analytical X-Ray Devices Module 9

Neutrinos with a cosmic ray detector. Cosmic rays with a neutrino detector

ECEN689: Special Topics in High-Speed Links Circuits and Systems Spring 2012

c. VH: Heating voltage between the collector and emitter.

Lecture 1: Applications of High Power Electromagnetic Systems

EE290C Spring Motivation. Lecture 6: Link Performance Analysis. Elad Alon Dept. of EECS. Does eqn. above predict everything? EE290C Lecture 5 2

ECE Microwave Engineering

Coherent Control of a Single Electron Spin with Electric Fields

Novel spectrum sensing schemes for Cognitive Radio Networks

THE random coupling model (RCM) makes predictions of

Experimental Characterization of Nonlinear Dynamics from Chua s Circuit

Mass of the electron m 0

MIL-STD-750D METHOD THERMAL RESISTANCE MEASUREMENTS OF GaAs MOSFET's (CONSTANT CURRENT FORWARD-BIASED GATE VOLTAGE METHOD)

Simulation of Secondary Electron Emission with CST PARTICLE STUDIO

Developing Quantum Logic Gates: Spin-Resonance-Transistors

Year 10 End of Year Examination Revision Checklist

Qualitative Studies with Microwaves

Workshop 2: Acoustic Output Measurements

A simple electronic circuit to demonstrate bifurcation and chaos

Ranging detection algorithm for indoor UWB channels

Qualitative Studies with Microwaves

SerDes_Channel_Impulse_Modeling_with_Rambus

Electric and magnetic fields, microwave therapy

EE194-EE290C. 28 nm SoC for IoT. Acknowledgement: Wayne Stark EE455 Lecture Notes, University of Michigan

Analyzing Uncertainty Matrices Associated with Multiple S-parameter Measurements

State Estimation and Motion Tracking for Spatially Diverse VLC Networks

Measurement of wakefields in hollow plasma channels Carl A. Lindstrøm (University of Oslo)

III. Spherical Waves and Radiation

Antenna measurements

The ATLAS Liquid Argon Calorimeter: Construction, Integration, Commissioning Ph. Schwemling on behalf of the ATLAS LAr Group

2D Periodic Surface Lattice Cherenkov maser experiment

ABSTRACT. Quantum graphs provide a setting to test the hypothesis that all ray-chaotic systems

CS6956: Wireless and Mobile Networks Lecture Notes: 2/4/2015

A RICH Photon Detector Module with G-APDs

This is a repository copy of Unite to build a quantum internet. White Rose Research Online URL for this paper:

WEEK 1 INTRO: MEASURING A GAUSSIAN BEAM. CALIBRATING YOUR PHOTODETECTOR

Interaction between surface acoustic waves and a transmon qubit

PMD Compensator and PMD Emulator

Omar M. Ramahi University of Waterloo Waterloo, Ontario, Canada

Parametric down-conversion

A MODIFIED CAUCHY METHOD SUITABLE FOR DUPLEXER AND TRIPLEXER RATIONAL MODELS EXTRACTION

Large Plasma Device (LAPD)

Universal Impedance Fluctuations in Wave Chaotic Systems. Steven M. Anlage 1,3

FATEK. FBs-1HLC. Precision Load Cell Module. Operation manual V1.1 06/07/2017 FATEK AUTOMATION CORP.

Plasma turbulence measured by fast sweep reflectometry on TORE SUPRA

Florent Lecocq. Control and measurement of an optomechanical system using a superconducting qubit. Funding NIST NSA/LPS DARPA.

XR Analog Clock - Manual Setting Model Troubleshooting Guide

Estimation of the Capacity of Multipath Infrared Channels

Harnessing Interaction in Bursty Interference Networks

A CALIBRATION PROCEDURE FOR TWO-PORT VNA WITH THREE MEASUREMENT CHANNELS BASED ON T-MATRIX

Vector dark domain wall solitons in a fiber ring laser

The Interaction Velocity of the Electric Force

Square Root Raised Cosine Filter

Development of Stripline Kicker for APS

Interactive Interference Alignment

Experimental and Simulated Chaotic RLD Circuit Analysis with the Use of Lorenz Maps

Quantum non-demolition measurements:

EE 474 Lab Part 2: Open-Loop and Closed-Loop Control (Velocity Servo)

POWER QUALITY MEASUREMENT PROCEDURE. Version 4 October Power-Quality-Oct-2009-Version-4.doc Page 1 / 12

First propositions of a lattice for the future upgrade of SOLEIL. A. Nadji On behalf of the Accelerators and Engineering Division

Transient Response of Transmission Lines and TDR/TDT

Module of Silicon Photomultipliers as a single photon detector of Cherenkov photons

St Olave s Physics Department. Year 11 Mock Revision Checklist

Interference and SINR in Dense Terahertz Networks

Physics: Waves, Sound/Light, Electromagnetic Waves, Magnetism, Mains Electricity and the National Grid

Deterministic Chaos Lab

Fundamentals of Low Intensity Shock Calibration

Fading Statistical description of the wireless channel

Supplementary Information. Holographic Detection of the Orbital Angular Momentum of Light with Plasmonic Photodiodes

Introduction Introduction

Simulations and Observations of GNSS Ocean Surface Reflections

Mapper & De-Mapper System Document

Matter Waves. Chapter 5

Aspects of the Scattering and Impedance Properties of Chaotic Microwave Cavities

CERN Accelerator School Wakefields. Prof. Dr. Ursula van Rienen, Franziska Reimann University of Rostock

D-D FUSION NEUTRONS FROM A STRONG SPHERICAL SHOCK WAVE FOCUSED ON A DEUTERIUM BUBBLE IN WATER. Dr. Michel Laberge General Fusion Inc.

Quasi-Optical Design and Analysis (MBI) Créidhe O Sullivan, J.Anthony Murphy, Marcin Gradziel, Neil Trappe, Tully Peacocke & graduate students

Design and Test of a PZT Wind Generator Excited by Rotary Magnet

Nonlinear Effects in Optical Fiber. Dr. Mohammad Faisal Assistant Professor Dept. of EEE, BUET

THz Electron Gun Development. Emilio Nanni 3/30/2016

RC & RL TRANSIENT RESPONSE

Electromagnetic Wave Absorption Technology for Stub Effects Mitigation

Computation of Electromagnetic Energy Absorption in the Human Body Tissues by High Frequency Structure Simulator

Optimum Transmission Scheme for a MISO Wireless System with Partial Channel Knowledge and Infinite K factor

Nonlinearity Equalization Techniques for DML- Transmission Impairments

Center for Spintronic Materials, Interfaces, and Novel Architectures. Voltage Controlled Antiferromagnetics and Future Spin Memory

GPR surveys at Nõmmküla Detection of underground water routes

Update on Timepix3 Telescope & Grazing Angles Results

Measurements of photon scattering lengths in scintillator and a test of the linearity of light yield as a function of electron energy

Maxime GUILLAUD. Huawei Technologies Mathematical and Algorithmic Sciences Laboratory, Paris

Transcription:

Time Reversed Electromagnetic Wave Propagation as a Novel Method of Wireless Power Transfer Frank Cangialosi, Tyler Grover, Patrick Healey, Tim Furman, Andrew Simon, Steven M. Anlage 1

Current State of Long-Range WPT Ubiquitous WPT requires greater range than provided by near-field technologies Microwave Beaming

Current State of Long-Range WPT Ubiquitous WPT requires greater range than provided by near-field technologies Microwave Beaming Precise Alignment Obstructions

Current State of Long-Range WPT Ubiquitous WPT requires greater range than provided by near-field technologies Microwave Beaming Precise Alignment Obstructions

Current State of Long-Range WPT Ubiquitous WPT requires greater range than provided by near-field technologies Microwave Beaming Precise Alignment Safety Hazard Obstructions

1. Time Forward Step Target requests power, source records sona Time Reversal A signal-focusing technique Target Device T S Voltage (mv) Power Source 15 1 5-5 -1-15 (Enclosed cavity with reflecting walls) 2 4 6 8 1 12 14

1. Time Forward Step Target requests power, source records sona Gaussian Pulse (5 ns) T Time Reversal A signal-focusing technique Target Device S Voltage (mv) Power Source 15 1 5-5 -1-15 (Enclosed cavity with reflecting walls) Sona" 2 4 6 8 1 12 14

Time Reversal A signal-focusing technique 1. Time Forward Step Target requests power, source records sona 2. Time Reverse Step Source reverses and broadcasts, sona reconstructs on target 4 3 2 1-1 -2-3 -4 13.45 13.46 13.47 13.48 13.4913.513.51 Time(µs) Target Device T S Voltage (mv) Power Source 15 1 5-5 -1-15 (Enclosed cavity with reflecting walls) Sona" 2 4 6 8 1 12 14

Time Reversal A signal-focusing technique 1. Time Forward Step 2. Time Reverse Step Target requests power, source records sona Source reverses and broadcasts, sona reconstructs on target 4 3 2 1-1 -2-3 -4 13.45 13.46 13.47 13.48 13.49 13.5 13.51 Target Device T Time(µs) Sona" 51 Voltage (mv) (Enclosed cavity 15 1 5 S Power Source -5-1 -15 with reflecting walls) 41 2 214 16 88 1 6 12 4 14 2 1 5 5151

Time Reversal A signal-focusing technique 1. Time Forward Step 2. Time Reverse Step Target requests power, source records sona Source reverses and broadcasts, sona reconstructs on target 4 3 2 1-1 -2-3 -4 13.45 13.46 13.47 13.48 13.49 13.5 13.51 Target Device T Reconstruction Time(µs) pulse Sona" 51 Voltage (mv) (Enclosed cavity 15 1 5 S Power Source -5-1 -15 with reflecting walls) 41 2 214 16 88 1 6 12 4 14 2 1 5 5151

Time Reversal A signal-focusing technique 1. Time Forward Step 2. Time Reverse Step Target requests power, source records sona Source reverses and broadcasts, sona reconstructs on target 4 3 2 1-1 -2-3 -4 13.45 13.46 13.47 13.48 13.49 13.5 13.51 Target Device T Reconstruction Time(µs) pulse Sona" (Enclosed cavity 51 Voltage (mv) Good for rectification 15 1 5 S Power Source -5-1 -15 with reflecting walls) 41 2 214 16 88 1 6 12 4 14 2 1 5 5151

Time Reversal for WPT Requires Provides 1 Spatial reciprocity of the wave equation 1 Range (not limited to free space drop-off) 2 Reflective surfaces 2 Resilience to obstructions 3 Ray-chaotic environment 3 Power concentrated at any given location 5

Experimental Setup Power Source (5Ghz, 3dBm) Scattering panels ensure ray chaos Device (on MikroMove) +35 (mm) -35 Wave Generation (TX) Wave Analysis (RX) PSG AWG MATLAB Oscilloscope 6

Spatial Profiling of Reconstruction +35 Target: mm -35 Constant Velocity.2 mm/s 7

Spatial Profiling of Reconstruction +35 Target: mm -35 Constant Velocity.2 mm/s 7

Spatial Profiling of Reconstruction +35 Target: mm -35 Constant Velocity.2 mm/s 7

Spatial Profiling of Reconstruction +35 Target: mm -35 Constant Velocity.2 mm/s 7

Spatial Profiling of Reconstruction x + c V (x) =a sinc b + d V (x) x 8

Spatial Profiling of Reconstruction x + c V (x) =a sinc b + d V (x) x 8

Spatial Profiling of Reconstruction x + c V (x) =a sinc b + d V (x) Background noise x 8

Spatial Profiling of Reconstruction x + c V (x) =a sinc b + d V (x) Background noise x 8

Targeting a Moving Receiver Refresh the sona before it gets stale Peak-To-Peak Voltage (V) 3.5 3 2.5 2 1.5 1.5 V(t) 2 4 6 8 1 12 14 Time (s) 9

Targeting a Moving Receiver Refresh the sona before it gets stale Peak-To-Peak Voltage (V) 3.5 3 2.5 2 1.5 1.5 V(t) 2 4 6 8 1 12 14 Time (s) 9

Targeting a Moving Receiver Refresh the sona before it gets stale Peak-To-Peak Voltage (V) 3.5 3 2.5 2 1.5 1.5 V(t) 2 4 6 8 1 12 14 Time (s) 9

Targeting a Moving Receiver Refresh the sona before it gets stale Peak-To-Peak Voltage (V) 3.5 3 2.5 2 1.5 1.5 V(t) 2 4 6 8 1 12 14 Time (s) 9

Targeting a Moving Receiver Refresh the sona before it gets stale Peak-To-Peak Voltage (V) 3.5 3 2.5 2 1.5 1.5 Dead time 2 4 6 8 1 12 14 Time (s) 9 V(t)

Targeting a Moving Receiver Refresh the sona before it gets stale Peak-To-Peak Voltage (V) 3.5 3 2.5 2 1.5 1.5 Dead time 2 4 6 8 1 12 14 Time (s) 9 V(t)

Targeting a Moving Receiver Refresh the sona before it gets stale Peak-To-Peak Voltage (V) 3.5 3 2.5 2 1.5 1.5 Experimental Results 2 4 6 8 1 12 14 Time (s) 1 V(t)

Potential WPT System Initialization Steady State Supplier searches for participating devices (which may or may not have charge) Small fraction of power reflected by device, allowing supplier to find new location Talk Session 5 Friday,17:45 (Selective Collapse of Nonlinear Time Reversed Electromagnetic Waves)

Limitations And Future Work Transfer efficiency Use multiple channels Environmental losses Investigate and mitigate Dead time Use dedicated hardware TX and calculate new sona simultaneously These limitations are dependent on our lab equipment, they are not fundamental limitations of the technique 12

Summary Time Reversal is a promising new basis for long-range WPT can transmit energy to receivers in motion does not require the receiver to be powered Poster Session 2 Friday,14:4 (Time Reversed Wave Propagation as a Novel Method of WPT) Talk Session 5 Friday,17:45 (Selective Collapse of Nonlinear Time Reversed Electromagnetic Waves) frank@cs.umd.edu anlage@umd.edu 13