Breakout Magnetics: How Far Can We Take the Next Generation of Components Weyman Lundquist President and CEO West Coast Magnetics ISO9001:2008 ISO13485.

Slides:



Advertisements
Similar presentations
Heat Generation in Electronics Thermal Management of Electronics Reference: San José State University Mechanical Engineering Department.
Advertisements

Phy 213: General Physics III Chapter 26: Electric Current Lecture Notes.
Why kicking Colombia out of the world cup could help keep the lights on in Rio “Easy energy efficiency gains through super low loss amorphous technology”
Inductors and Chokes In Switch mode Supplies
SWITCH-MODE POWER SUPPLIES AND SYSTEMS Silesian University of Technology Faculty of Automatic Control, Electronics and Computer Sciences Ryszard Siurek.
Copyright (c) LBRGroup All Rights Reserved. 1 MARKET PROFILE CONCEPTS Ways of organizing activity and structure “There is no greater indicator.
Ch6 DC-DC Converters 6-1 Linear voltage regulators Fig. 6.1 Adjustingbasecurrent, => linear DC-DC converter orlinear regulator Thetransistor operates in.
UNIT 13 : HEAT 13.1 Thermal Conductivity 13.2 Thermal Expansion.
Senior Design Project Team John Kmiec John Pipitone Project Advisor Dr. Lili He LED Based Track Lighting System San Jose State University Senior Project.
Switching Power Supply Component Selection 7.2a Inductor Selection – Terminology.
Magnetics Design Primary Constraints: Peak Flux Density (B field) in the core : B max (T or Wb/m 2 ) Core losses Saturation Peal Current density in the.
ELECTRIC CIRCUIT ANALYSIS - I
Study at Mid Sweden University1 High Speed Switched Mode Power Supplies Kent Bertilsson Mid-Sweden University SEPS Technologies AB Small Efficient.
Overview of different wind generator systems and their comparisons 2-4~2-7 陳昱希.
Switchmode Transformer Design By: Rizwan Khalid. Outline Introduction Theory Pexpert simulations Applications Conclusion.
Bridge Converters and Faraday Screens By Paul Wilson.
04/09/02EECS 3121 Lecture 25: Interconnect Modeling EECS 312 Reading: 8.3 (text), 4.3.2, (2 nd edition)
Institute of Digital and Computer Systems 1 Fabio Garzia / Finding Peak Performance in a Process23/06/2015 Chapter 5 Finding Peak Performance in a Process.
WINDING LOSSES IN HIGH FREQUENCY TRANSFORMERS
Workshop on Special Compact and Low Consumption Magnet Design
Foil Windings in Power Inductors: Methods of Reducing AC Resistance
Magnetics Design Primary Constraints:
Low AC and DC Resistance Inductor Technology Weyman Lundquist – President and CEO West Coast Magnetics April 4, 2007 International Patent # WO 2005/09630.
Chapter 3Transmission Lines Why use high-voltage transmission lines? The best answer to that question is that high-voltage transmission lines transport.
DC-DC Fundamentals 1.3 Switching Regulator
BASIC CONSIDERATIONS IN DESIGN  The aim of the design is to completely obtain the dimensions of all the parts of the machine to furnish the data to the.
Switching Power Supply Component Selection 7.2b Inductor Selection – Application.
Life’s Ultimate Problem… Solved By…. Preliminary Design Review Team Iron Chefs Ahmad Alawadhi Eric Willuweit Kegan Grimes Kyle Chessman Sean Flodberg.
Chapter 22 Alternating-Current Circuits and Machines.
W10D1: Inductance and Magnetic Field Energy
CHAPTER 6: TRANSFORMER BAKISS HIYANA ABU BAKAR
Power Electronics and Drives (Version ) Dr. Zainal Salam, UTM-JB 1 Chapter 3 DC to DC CONVERTER (CHOPPER) General Buck converter Boost converter.
DC-DC Buck Converter in Inner Detector Environment
CHAPTER 16 Power Circuits: Switching and Amplifying.
October 15, 2008 DC Circuits. This is the week that will have been Today Complete Resistance/Current with some problems Friday Examination #2: Potential.
Fundamental Antenna Parameters
Wim Schoenmaker ©magwel2005 Electromagnetic Modeling of Back-End Structures on Semiconductors Wim Schoenmaker.
ELECTRICAL BASICS (Chapter 8) Electrical terms Electricity & magnetism Electricity Circuits Magnetism Electrical units Electric potential or eletromotive.
Section 3 Basic Electricity and Magnetism
Chapter 27 Current and Resistance. Intro Up until now, our study of electricity has been focused Electrostatics (charges at equilibrium conditions). We.
SWITCH-MODE POWER SUPPLIES AND SYSTEMS Silesian University of Technology Faculty of Automatic Control, Electronics and Computer Sciences Ryszard Siurek.
Induction Motors.
Application of the Electrothermal Average Inductor Model for Analyses of Boost Converters Krzysztof Górecki, Janusz Zarębski, Kalina Detka Gdynia Maritime.
Chapter 27 Current and Resistance Scalar Sense determined by the movement of the positive charge carrier Average Electric Current Instantaneous Electric.
Nelson Research, Inc – N. 88 th St. Seattle, WA USA aol.com Non-Contacting Eddy Current Conductivity Sensor for Measuring.
Induction Machine The machines are called induction machines because of the rotor voltage which produces the rotor current and the rotor magnetic field.
Level 3 Practical Investigation Where to start?. Aim This is the purpose of your practical i.e. what it is that you want to find out This is the purpose.
TECHNICAL ANALYSIS. PRICE PATTERNS A typical price cycle has three trends: up, sideways, and down. The sideways trend is essentially a horizontal or.
Section 3: Basic Automatic Controls Unit 12: Basic Electricity and Magnetism.
Prof R T Kennedy1 EET 423 POWER ELECTRONICS -2. Prof R T Kennedy2 IDEAL TRANSFORMER MAGNETIC DEVICE ELECTRICAL ISOLATION FUNCTION: TRANSFER ENERGY SCALE.
EET 423 POWER ELECTRONICS -2
The Different Types of Inductors and Their Affecting Factors
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Parul Institute Of Technology Name Of Subject:-Electrical Machines Name Of Faculty:-(1) Suresh Sahoo (2) Yogendra Tiwari E&C 3 rd Sem. Prepaid By :- Sr.No.NameEnrolment.
HNC/D Engineering Science
Heat Sinks and Component Temperature Control
EET 423 POWER ELECTRONICS -2
BASIC ELECTRICAL TECHNOLOGY Chapter 4 – Magnetic Circuits
Dual Active Bridge Series Resonant Converter with Pulse Modulation
PExprt Modeling Procedure
Electric Machine Induction Motor
Magnetic Circuits.
Krzysztof Górecki and Kalina Detka
Experiment 3 Part A: Making an Inductor
Circuit Components.
Electron Collider Ring Magnets Preliminary Summary
T- Norah Ali Al- moneef king Saud university
Electric Machine Design Course
Presentation transcript:

Breakout Magnetics: How Far Can We Take the Next Generation of Components Weyman Lundquist President and CEO West Coast Magnetics ISO9001:2008 ISO13485 Registered

Outline Where do device losses come from? How much improvement is available from packaging? Core material improvements, and future forecast. How much power density improvement is available today? What is the forecast for winding losses? What can we expect from increasing the operating frequency? Where will we be in 10 years? Where are we headed in 20 years+?.

How Much Better Can we Get? How Quickly? Assumptions to Work From This presentation considers transformers operating at SMPS frequencies although many of the same conclusions will apply to inductors. This trend analysis assumes that designs will be optimal, I am not considering the effect of non-optimal designs, which is considerable. Let’s assume we are going to design to a given temperature rise and see how far we can reduce the device size. I will define a device by its power handling capability divided by total volume of the device (holding temperate rise constant). Transformer sizes for purposes of this presentation are based on kHz 1-5 kW designs.

Where do Losses Come From? Typical 1500 W Transformer, 250 kHz Core Loss: 4 Watts Winding Loss: 3 Watts Total Loss: 7 Watts Efficiency 99.5%! Core cross sectional area (Ae)

Effective Use of Available Volume Current Typical ETD49 New Design Full Cube = L x W x H = 101 cm3 Watts/cm3 = 11.2 * Full Cube = L x W x H = 91 cm3 Watts/cm3 = 16.5 * Improvement Available Today = 47% * Power rating based on constant temperature rise design same core and winding technology used for each device.

What is the Potential for Improved Packaging? % of Total Device Cube That is Core Volume and Winding Volume Only Improvements to 80% or higher will be possible with improved insulating materials and better use of existing materials.

Core Losses Conclude: we want to decrease the product of Ae and N or increase the product of B and F without increasing core loss density.

What Does the Future Hold for Improved Core Materials? 4.7% avg. annual reduction in core loss from 1969 to 3C98 introduction in Source: Ferroxcube, Core Loss at 1 kGauss, 100 kHz

What Core Materials are Being Chosen for Today’s Designs Stocking Quantities through U.S. Distribution Year of Introduction The presenter is certain that many new designs use core materials from 10+ old releases Improvement available today: 50%

Improvement Available Today – More Efficient Packaging and Lower Loss Core Full Cube = L x W x H = 101 cm3 Watts = 2400 at 100 kHz Watts/cm3 = 23.7 Full Cube = L x W x H = 91 cm3 Watts = 4300 at 100 kHz Watts/cm3 = 47.3 IMPROVEMENT 2.0 times power density

How About Winding Losses, What Can We Expect in the Future? Copper and Aluminum are going to remain the materials of choice for at least 10 years. Good News: Cu and Al have relatively low resistivity and low cost. Good News: Litz wire can be used to manage high frequency winding losses up to about 1 MHz without an increasing penalty to DCR Bad News: Not much improvement forecast for winding loss, and the problem above 1 MHz requires new solutions (not litz)

What About the Effect of Increasing the Operating Frequency? Source: Ferroxcube

Device Size vs. Frequency – State of the Art Today

10 Year Forecast 38% overall reduction in device volume Operating frequency will increase more quickly at 10% per year. This will result in an additional 30% reduction in device volume. Conclude: we can expect a decrease in device volume or increase in power density of at least 50% over the next 10 years as a result of better core materials and increased operating frequencies.

Further Out Approaching 20 Years and Beyond Approaching 20 years I expect to see device sizes in the range 20% to 30% of today’s volumes from more efficient use of available volume, improved core technology, improved winding technology and increasing frequency of operation to the 1 MHz range. Current ferrite core technology does not lead to reduced device size over 1.5 MHz. Litz wire is too costly and makes poor use of winding area for gauges suitable for frequencies over 1.5 MHz. Development of new core materials, and new winding technologies is needed or device size will plateau as we approach the 20 year mark. This development will happen.

Conclusions For many designs it is possible to double the power density with material options available today. Over the next 10 years it is expected average device volume will be cut in half due to improvements in core materials and increases in switching frequencies. This improvement is expected to extend out to 20 years with device sizes as small as 20% of todays typical devices. From 1.5 MHz to 10 MHz more development work is needed for further size reduction on both the core material side and the winding side. This is expected to occur.

Thank you for your time Weyman Lundquist, President West Coast Magnetics 4848 Frontier Way, Ste 100 Stockton, CA