Minntronix Technical Note Inductance measurement using real-world inductance bridges – or – What you ‘set’ may not be what you ‘get’ Dave LeVasseur VP.

Slides:



Advertisements
Similar presentations
AP Physics C Montwood High School R. Casao
Advertisements

Introductory Circuit Analysis Robert L. Boylestad
Kit Building Class Lesson 4Page 1 R and X in Series Inductors and capacitors resist the flow of AC. This property is called reactance. Resistance also.
High Frequency Saturable Reactor
Physics 2112 Unit 21  Resonance  Power/Power Factor  Q factor  What is means  A useful approximation  Transformers Outline:
DC Choppers 1 Prof. T.K. Anantha Kumar, E&E Dept., MSRIT
EE20A - Electromechanical Energy Conversion Induction Machine
SYNCHRONOUS GENERATORS
Sinusoidal Steady-State Power Calculations
Switchmode Transformer Design By: Rizwan Khalid. Outline Introduction Theory Pexpert simulations Applications Conclusion.
EE 311: EE Junior Lab Experiment 5 - Single Phase Transformers J. Carroll 9/25/06.
Duty Ratio Controlled Push Pull Converter
TSF Ferrite International Composite Cores Offer the Best of All Worlds George Orenchak TSC International.
Copyright by UNIT III DC Choppers 4/17/2017 Copyright by
Consider a long solenoid of cross-sectional area A, with number of turns N, and of length l. The flux is The magnitude of B is given by: Therefore, The.
Minntronix Technical Note
Problem Solving Part 2 Resonance.
EKT214 - ANALOG ELECTRONIC CIRCUIT II
Alternating Current Circuits
ECE 2300 Circuit Analysis Dr. Dave Shattuck Associate Professor, ECE Dept. Lecture Set #24 Real and Reactive Power W326-D3.
Ch. 30 Inductance AP Physics. Mutual Inductance According to Faraday’s law, an emf is induced in a stationary circuit whenever the magnetic flux varies.
Electrical Machine-I EE 2107 Dr. Md. Sherajul Islam
Chapter 9 Ideal Transformer
Introduction to Transistors
electronics fundamentals
Alternating Current Circuits
Chapter 31 Electromagnetic Oscillations and Alternating Current Key contents LC oscillations, RLC circuits AC circuits (reactance, impedance, the power.
Electromagnetic Oscillations and Alternating Current
Alternating Current Circuits
Chapter 11 AC Steady-State Power
ELECTRICAL ENGINEERING: PRINCIPLES AND APPLICATIONS, Fourth Edition, by Allan R. Hambley, ©2008 Pearson Education, Inc. Lecture 9 Op-Amp Circuits.
Chapter 13 Principles of Electric Circuits, Conventional Flow, 9 th ed. Floyd © 2010 Pearson Higher Education, Upper Saddle River, NJ All Rights.
DC/AC Fundamentals: A Systems Approach
Fundamentals of Electromagnetics and Electromechanics
Announcements For lectures 8 to 10 please be reading Chapter 3
Transformer Model where r = diag [r 1 r 2 ], a diagonal matrix, and The resistances r 1 and r 2 and the flux linkages l 1 and l 2 are related to coils.
10/11/2015 Operational Amplifier Characterization Chapter 3.
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 6-1 Electronics Principles & Applications Eighth Edition Chapter 6 Introduction.
Inductors An inductor is essentially a coil of wire with an iron core.
Introduction  The fundamental passive linear circuit elements are the  resistor (R),  capacitor (C)  inductor (L).  These circuit.
Chapter 13 Principles of Electric Circuits, Conventional Flow, 9 th ed. Floyd © 2010 Pearson Higher Education, Upper Saddle River, NJ All Rights.
Today Course overview and information 09/16/2010 © 2010 NTUST.
Physics 212 Lecture 21, Slide 1 Physics 212 Lecture 21.
Chapter 31 Lecture 33: Alternating Current Circuits: II HW 11 (problems): 30.58, 30.65, 30.76, 31.12, 31.26, 31.46, 31.56, Due Friday, Dec 11. Final.
Chapter 8 Alternating Current Circuits. AC Circuit An AC circuit consists of a combination of circuit elements and an AC generator or source An AC circuit.
Lecture 18 Chapter 32 Outline Gauss Law for Mag Field Maxwell extension of Ampere’s Law Displacement Current Spin/ Orbital Mag Dipole Moment Magnetic Properties.
1 ELECTRICAL TECHNOLOGY EET 103/4 Define and analyze the principle of transformer, its parameters and structure. Describe and analyze Ideal transformer,
1 ELECTRICAL TECHNOLOGY EET 103/4 Define and analyze the principle of transformer, its parameters and structure. Describe and analyze Ideal transformer,
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
- Minntronix Technical Note - Effects of Air Gap Tolerance on Inductance Tolerance Dave LeVasseur VP of Research & Development Minntronix, Inc. 4-Mar-2016.
Diode Circuit Analysis
About the different types of variables, How to identify them when doing your practical work. Learning Objectives You should learn :
Part Three – Relay Input Sources
Chapter 11 Electronics Fundamentals Circuits, Devices and Applications - Floyd © Copyright 2007 Prentice-Hall Chapter 11.
Electrical impedance Electrical impedance, or simply impedance, describes a measure of opposition to alternating current (AC). Electrical impedance extends.
Amplifier: An amplifier is an electronic device that increases voltage, current or power of a signal. According to the class of operation, the amplifiers.
Real and Reactive Power
Testing of Transformers
Learning Objectives You should learn :
Minntronix Technical Note
An {image} series circuit has {image} , {image} , and {image}
UNIT 2 Magnetic Circuits
Variables are things that vary and change
19 Inductance Chapter Topics Covered in Chapter 19
Learning Objectives You should learn :
Learning Objectives You should learn :
Alternating Current Circuits
Learning Objectives You should learn :
Electric Machine Design Course
Presentation transcript:

Minntronix Technical Note Inductance measurement using real-world inductance bridges – or – What you ‘set’ may not be what you ‘get’ Dave LeVasseur VP of Research & Development Minntronix, Inc. 17-Dec-14

The Problems: Setting the drive level on many inductance bridges doesn’t always guarantee that the level you set will be the same as what is applied to the part under test. Most if not all core materials (except for “air”) exhibit changes in their permeability at different drive levels. When tested near its saturation point the inductance of a winding may vary widely causing some bridges to provide erroneous readings or no reading at all.

Part 1: How inductance bridges work Like any oscillator or amplifier all inductance bridges have an internal driving impedance, shown here as R int. The amount of voltage that will appear across the inductor under test, shown here as V ut and Z ut depend on the relative values of R int and Z ut. When Z ut >> R int the voltage across Z ut will be almost the same as V set. Z ut R int V set bridge V ut

When Z ut = R int the voltage across Z ut will be half of V set. When Z ut << R int then the voltage appearing across Z ut will be much less than V set. The value of V ut is based on the voltage splitting principle: Z ut R int V set bridge V ut Part 1: How inductance bridges work

Determining the internal impedance and applied drive voltage capabilities of the Wayne Kerr WK3260B based on empirical measurements. DJL6-Dec-14 ALC=offf=1kHzZut = 50 ohm max variable resistor load VsetVmZutIut (calc)Zint (ohms)Pout (mW) Average:48.16ohms A Real-World Example The first step: verify the internal impedance of the inductance bridge

A real-world example The second step: measure an impedance, verify the results We can see in this case that setting a voltage of 100mV nets around a third of that to the inductor under test. *Complex math operators are required to obtain correct results.

Part 2: How drive level affects inductance The permeability versus flux density curve of a typical high- perm (10K u) ferrite, in this case Mag Inc “W” material, shows how permeability can be a strong function of drive level when driven near saturation. Mag Inc lists B sat for their “W” as 4300 gauss. At room temperature the permeability rises from 100% at low drive levels to 125% at around 1500 gauss then drops off as drive level increases toward saturation. The effect is more pronounced at elevated temperatures.

Part 2: How drive level affects inductance Core manufacturers usually specify relatively low drive levels for their test condition. This slide shows a core spec to be tested at 5 gauss (0.5mT). It is for this reason that we transformer manufacturers are reluctant to specify inductance limits that are based strictly on the AL value and its tolerance without first checking the core’s test specs. The next slide shows why…

Part 2: How drive level affects inductance

A real-world example The second step, continued: measure an impedance, verify the results Returning to our example, with V set = 1.0V the inductor now reads 3.846mH with Q=5.794 resulting in an impedance of j23.42Ω. The voltage being applied to the inductor becomes: Since the inductance increased due to higher permeability the voltage splitting factor also increased resulting in a higher proportion of drive level across the inductor.

A real-world example So why won’t my inductance bridge provide a reading? Borrowing (shamelessly) from a Wayne-Kerr equipment manual shows how the operating point of an inductor being subjected to high drive levels is effectively taking an average of the core’s permeability. If the inductance bridge tries to ‘set’ the voltage at a given value based on an impedance that is changing it may never be able to settle on a consistent reading. This ‘hunting’ process slows down production testing which is why most production engineers avoid using ALC except when absolutely necessary.

A real-world example What to do about it?

References: – source for background on inductance bridges - Complex Math Calculator Also: Complex Calc, Android App by Renat NotfullinComplex Calc