Dissipation Factor, Power Factor, and Relative Permittivity (Dielectric Constant)
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Basic PCB Material Electrical and Thermal Properties for Design Introduction
1 Basic PCB material electrical and thermal properties for design Introduction: In order to design PCBs intelligently it becomes important to understand, among other things, the electrical properties of the board material. This brief paper is an attempt to outline these key properties and offer some descriptions of these parameters. Parameters: The basic ( and almost indispensable) parameters for PCB materials are listed below and further described in the treatment that follows. dk, laminate dielectric constant df, dissipation factor Dielectric loss Conductor loss Thermal effects Frequency performance dk: Use the design dk value which is assumed to be more pertinent to design. Determines such things as impedances and the physical dimensions of microstrip circuits. A reasonable accurate practical formula for the effective dielectric constant derived from the dielectric constant of the material is: -1/2 εeff = [ ( εr +1)/2] + [ ( εr -1)/2][1+ (12.h/W)] Here h = thickness of PCB material W = width of the trace εeff = effective dielectric constant εr = dielectric constant of pcb material df: The dissipation factor (df) is a measure of loss-rate of energy of a mode of oscillation in a dissipative system. It is the reciprocal of quality factor Q, which represents the Signal Processing Group Inc., technical memorandum. Website: http://www.signalpro.biz. Signal Processing Gtroup Inc., designs, develops and manufactures analog and wireless ASICs and modules using state of the art semiconductor, PCB and packaging technologies. For a free no obligation quote on your product please send your requirements to us via email at [email protected] or through the Contact item on the website. -
Uprating of Electrolytic Capacitors
White Paper Uprating of Electrolytic Capacitors By Joelle Arnold Uprating of Electrolytic Capacitors Aluminum electrolytic capacitors are comprised of two aluminum foils, a cathode and an anode, rolled together with an electrolyte-soaked paper spacer in between. An oxide film is grown on the anode to create the dielectric. Aluminum electrolytic capacitors are primarily used to filter low-frequency electrical signals, primarily in power designs. The critical functional parameters for aluminum electrolytic capacitors are defined as capacitance (C), leakage current (LC), equivalent series resistance (ESR), impedance (Z), and dissipation factor (DF). These five parameters are interrelated through the following schematic. Physically, leakage current (LC) tends to be primarily driven by the behavior of the dielectric. ESR is primarily driven by the behavior of the electrolyte. Physically, impedance (Z) is a summation of all the resistances throughout the capacitor, including resistances due to packaging. Electrically, Z is the summation of ESR and either the capacitive reactance (XC), at low frequency, or the inductance (LESL), at high frequency (see Figure 1). Dissipation factor is the ratio of ESR over XC. Therefore, a low ESR tends to give a low impedance and a low dissipation factor. 1.1 Functional Parameters (Specified in Datasheet) The functional parameters that can be provided in manufacturers’ datasheets are listed below 1.1.1 Capacitance vs. Temperature It can be seen that the manufacturer’s guarantee of ±20% stability of the capacitance is only relevant at room temperature. While a source of potential concern when operating aluminum electrolytic capacitors over an extended temperature range, previous research has demonstrated that the capacitance of this capacitor is extremely stable as a function of temperature (see Figure 2 and Figure 4). -
Equivalent Series Resistance (ESR) of Capacitors
Application Note 1 of 5 Equivalent Series Resistance (ESR) of Capacitors Questions continually arise concerning the correct definition of the ESR (Equivalent Series Resistance) of a capacitor and, more particularly, the difference between ESR and the actual physical series resistance (which we'll call Ras), the ohmic resistance of the leads and plates or foils. The definition and application of the term ESR has often been misconstrued. We hope this note will answer any questions and clarify any confusion that might exist. Very briefly, ESR is a measure of the total lossiness of a capacitor. It is larger than Ras because the actual series resistance is only one source of the total loss (usually a small part). The Series Equivalent Circuit At one frequency, a measurement of complex impedance gives two numbers, the real part and the imaginary part: Z = Rs + jXs. At that frequency, the impedance behaves like a series combination of an ideal resistance Rs and an ideal reactance Xs (Figure 1). Rs RS XS CS Figure 1: Equivalent series circuit representation If Xs is negative, the impedance is capacitive, and the general reactance can be replaced with a capacitance of: −1 Cs = ωXs We now have an equivalent circuit that is correct only at the measurement frequency. The resistance of this equivalent circuit is the equivalent series resistance ESR = Rs = Real part of Z © IET LABS, Inc., September 2019 Printed in U.S.A 035002 Rev. A4 1 of 5 Application Note 2 of 5 Add the dissipation FACTOR energy lost Real part of Z If we define the dissipation factor D as D = = energy stored (− Imaginary part of Z) Rs Then D = =Rsω C = (ESR) ω C (− )Xs If one took a pure resistance and a pure capacitance and connected them in series, then one could say that the ESR of the combination was indeed equal to the actual series resistance. -
Agilent Basics of Measuring the Dielectric Properties of Materials
Agilent Basics of Measuring the Dielectric Properties of Materials Application Note Contents Introduction ..............................................................................................3 Dielectric theory .....................................................................................4 Dielectric Constant............................................................................4 Permeability........................................................................................7 Electromagnetic propagation .................................................................8 Dielectric mechanisms ........................................................................10 Orientation (dipolar) polarization ................................................11 Electronic and atomic polarization ..............................................11 Relaxation time ................................................................................12 Debye Relation .................................................................................12 Cole-Cole diagram............................................................................13 Ionic conductivity ............................................................................13 Interfacial or space charge polarization..................................... 14 Measurement Systems .........................................................................15 Network analyzers ..........................................................................15 Impedance analyzers and LCR meters.........................................16 -
Application Note: ESR Losses in Ceramic Capacitors by Richard Fiore, Director of RF Applications Engineering American Technical Ceramics
Application Note: ESR Losses In Ceramic Capacitors by Richard Fiore, Director of RF Applications Engineering American Technical Ceramics AMERICAN TECHNICAL CERAMICS ATC North America ATC Europe ATC Asia [email protected] [email protected] [email protected] www.atceramics.com ATC 001-923 Rev. D; 4/07 ESR LOSSES IN CERAMIC CAPACITORS In the world of RF ceramic chip capacitors, Equivalent Series Resistance (ESR) is often considered to be the single most important parameter in selecting the product to fit the application. ESR, typically expressed in milliohms, is the summation of all losses resulting from dielectric (Rsd) and metal elements (Rsm) of the capacitor, (ESR = Rsd+Rsm). Assessing how these losses affect circuit performance is essential when utilizing ceramic capacitors in virtually all RF designs. Advantage of Low Loss RF Capacitors Ceramics capacitors utilized in MRI imaging coils must exhibit Selecting low loss (ultra low ESR) chip capacitors is an important ultra low loss. These capacitors are used in conjunction with an consideration for virtually all RF circuit designs. Some examples of MRI coil in a tuned circuit configuration. Since the signals being the advantages are listed below for several application types. detected by an MRI scanner are extremely small, the losses of the Extended battery life is possible when using low loss capacitors in coil circuit must be kept very low, usually in the order of a few applications such as source bypassing and drain coupling in the milliohms. Excessive ESR losses will degrade the resolution of the final power amplifier stage of a handheld portable transmitter image unless steps are taken to reduce these losses. -
Dielectric Loss
Dielectric Loss - εr is static dielectric constant (result of polarization under dc conditions). Under ac conditions, the dielectric constant is different from the above as energy losses have to be taken into account. - Thermal agitation tries to randomize the dipole orientations. Hence dipole moments cannot react instantaneously to changes in the applied field Æ losses. - The absorption of electrical energy by a dielectric material that is subjected to an alternating electric field is termed dielectric loss. - In general, the dielectric constant εr is a complex number given by where, εr’ is the real part and εr’’ is the imaginary part. Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - Consider parallel plate capacitor with lossy dielectric - Impedance of the circuit - Thus, admittance (Y=1/Z) given by Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - The admittance can be written in the form The admittance of the dielectric medium is equivalent to a parallel combination of - Note: compared to parallel an ideal lossless capacitor C’ with a resistance formula. relative permittivity εr’ and a resistance of 1/Gp or conductance Gp. Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - Input power: - Real part εr’ represents the relative permittivity (static dielectric contribution) in capacitance calculation; imaginary part εr’’ represents the energy loss in dielectric medium. - Loss tangent: defined as represents how lossy the material is for ac signals. Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss The dielectric loss per unit volume: Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - Note that the power loss is a function of ω, E and tanδ. -
A Comprehensive Guide to Selecting the Right Capacitor for Your Specific Application
CAPACITOR FUNDAMENTALS EBOOK A Comprehensive Guide to Selecting the Right Capacitor for Your Specific Application 2777 Hwy 20 (315) 655-8710 [email protected] Cazenovia, NY 13035 knowlescapacitors.com CAPACITOR FUNDAMENTALS EBOOK TABLE OF CONTENTS Introduction .................................. 2 The Key Principles of Capacitance and How a Basic Capacitor Works .............................. 3 How Capacitors are Most Frequently Used in Electronic Circuits ............................. 6 Factors Affecting Capacitance .................. 9 Defining Dielectric Polarization .................. 11 Dielectric Properties ........................... 15 Characteristics of Ferroelectric Ceramics ......................... 19 Characteristics of Linear Dielectrics .............. 22 Dielectric Classification ......................... 24 Test Parameters and Electrical Properties .......... 27 Industry Test Standards Overview. 32 High Reliability Testing .......................... 34 Visual Standards For Chip Capacitors ............. 37 Chip Attachment and Termination Guidelines ...... 42 Dissipation Factor and Capacitive Reactance ..... 49 Selecting the Right Capacitor for Your Specific Application Needs ............................ 51 1 CAPACITOR FUNDAMENTALS EBOOK INTRODUCTION At Knowles Precision Devices, our expertise in capacitor technology helps developers working on some of the world’s most demanding applications across the medical device, military and aerospace, telecommunications, and automotive industries. Thus, we brought together our top engineers -
LOSSY CAPACITORS 1 Dielectric Loss
Chapter 3—Lossy Capacitors 3–1 LOSSY CAPACITORS 1 Dielectric Loss Capacitors are used for a wide variety of purposes and are made of many different materials in many different styles. For purposes of discussion we will consider three broad types, that is, capacitors made for ac, dc, and pulse applications. The ac case is the most general since ac capacitors will work (or at least survive) in dc and pulse applications, where the reverse may not be true. It is important to consider the losses in ac capacitors. All dielectrics (except vacuum) have two types of losses. One is a conduction loss, representing the flow of actual charge through the dielectric. The other is a dielectric loss due to movement or rotation of the atoms or molecules in an alternating electric field. Dielectric losses in water are the reason for food and drink getting hot in a microwave oven. One way of describing dielectric losses is to consider the permittivity as a complex number, defined as = − j = ||e−jδ (1) where = ac capacitivity = dielectric loss factor δ = dielectric loss angle Capacitance is a complex number C∗ in this definition, becoming the expected real number C as the losses go to zero. That is, we define C∗ = C − jC (2) One reason for defining a complex capacitance is that we can use the complex value in any equation derived for a real capacitance in a sinusoidal application, and get the correct phase shifts and power losses by applying the usual rules of circuit theory. This means that most of our analyses are already done, and we do not need to start over just because we now have a lossy capacitor. -
Electrical and Capacitive Methods for Detecting Degradation in Wire Insulation Robert Thomas Sheldon Iowa State University
Iowa State University Capstones, Theses and Graduate Theses and Dissertations Dissertations 2012 Electrical and capacitive methods for detecting degradation in wire insulation Robert Thomas Sheldon Iowa State University Follow this and additional works at: https://lib.dr.iastate.edu/etd Part of the Electrical and Electronics Commons, and the Mechanics of Materials Commons Recommended Citation Sheldon, Robert Thomas, "Electrical and capacitive methods for detecting degradation in wire insulation" (2012). Graduate Theses and Dissertations. 12681. https://lib.dr.iastate.edu/etd/12681 This Thesis is brought to you for free and open access by the Iowa State University Capstones, Theses and Dissertations at Iowa State University Digital Repository. It has been accepted for inclusion in Graduate Theses and Dissertations by an authorized administrator of Iowa State University Digital Repository. For more information, please contact [email protected]. Electrical and capacitive methods for detecting degradation in wire insulation by Robert T. Sheldon A thesis submitted to the graduate faculty in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE Major: Electrical Engineering Program of Study Committee: Nicola Bowler, Major Professor Brian K. Hornbuckle Jiming Song Iowa State University Ames, Iowa 2012 Copyright c Robert T. Sheldon, 2012. All rights reserved. ii To my parents, Kevin and Victoria, and my sister, Laura, for their neverending love and support. iii TABLE OF CONTENTS LIST OF TABLES . vi LIST OF FIGURES . vii ABSTRACT . xii CHAPTER 1. GENERAL INTRODUCTION . 1 1.1 Introduction . .1 1.2 Literature survey . .1 1.2.1 Extant methods of insulation characterization . .1 1.2.2 Capacitive sensing . -
A Review of Degradation Behavior and Modeling of Capacitors: Preprint
A Review of Degradation Behavior and Modeling of Capacitors Preprint Anunay Gupta,1 Om Prakash Yadav,1 Douglas DeVoto,2 2 and Joshua Major 1 North Dakota State University 2 National Renewable Energy Laboratory Presented at the American Society of Mechanical Engineers (ASME) 2018 International Technical Conference and Exhibition on Packaging and Integration of Electronic and Photonic Microsystems (InterPACK 2018) San Francisco, California August 27–30, 2018 NREL is a national laboratory of the U.S. Department of Energy Conference Paper Office of Energy Efficiency & Renewable Energy NREL/CP-5400-71386 Operated by the Alliance for Sustainable Energy, LLC October 2018 This report is available at no cost from the National Renewable Energy Laboratory (NREL) at www.nrel.gov/publications. Contract No. DE-AC36-08GO28308 A Review of Degradation Behavior and Modeling of Capacitors Preprint Anunay Gupta,1 Om Prakash Yadav,1 Douglas DeVoto,2 2 and Joshua Major 1 North Dakota State University 2 National Renewable Energy Laboratory Suggested Citation Anunay Gupta, Om Prakash Yadav, Douglas DeVoto, and Joshua Major. 2018. A Review of Degradation Behavior and Modeling of Capacitors: Preprint. Golden, CO: National Renewable Energy Laboratory. NREL/CP-5400-71386. https://www.nrel.gov/docs/fy19osti/71386.pdf. NREL is a national laboratory of the U.S. Department of Energy Conference Paper Office of Energy Efficiency & Renewable Energy NREL/CP-5400-71386 Operated by the Alliance for Sustainable Energy, LLC October 2018 This report is available at no cost from the National Renewable Energy National Renewable Energy Laboratory Laboratory (NREL) at www.nrel.gov/publications. 15013 Denver West Parkway Golden, CO 80401 Contract No. -
Table of Contents
NOVACAP TECHNICAL BROCHURE Table of Contents A. INTRODUCTION ................................................................................................ 2 B. CAPACITOR APPLICATIONS ......................................................................... 3 C. THE BASIC CAPACITOR ................................................................................. 4 D. CAPACITANCE ................................................................................................... 5 E. FACTORS AFFECTING CAPACITANCE ...................................................... 5 F. DIELECTRIC BEHAVIOR ................................................................................. 7 G. DIELECTRIC PROPERTIES ......................................................................... 13 H. FERROELECTRIC CERAMICS.................................................................... 20 I. LINEAR DIELECTRICS ................................................................................... 24 J. CLASSES OF DIELECTRICS ......................................................................... 25 K. TEST PARAMETERS AND ELECTRICAL PROPERTIES...................... 29 L. INDUSTRY TEST STANDARDS..................................................................... 35 M. HIGH RELIABILITY TESTING .................................................................... 37 N. VISUAL STANDARDS FOR CHIP CAPACITORS ..................................... 40 O. CHIP USER GUIDELINES ............................................................................... 46 1 NOVACAP -
For Most Practical Waveguides the Loss Associated with Dielectric Loss
Adapted from notes by ECE 5317-6351 Prof. Jeffery T. Williams Microwave Engineering Fall 2019 Prof. David R. Jackson Dept. of ECE Notes 7 Waveguiding Structures Part 2: Attenuation ε,, µσ 1 Attenuation on Waveguiding Structures For most practical waveguides and transmission lines the loss associated with dielectric loss and conductor loss is relatively small. To account for these losses we will make this approximation: αα≈+cd α Attenuation constant Attenuation constant due due to conductor loss to dielectric loss (ignore dielectric loss) (ignore conductor loss) 2 Attenuation due to Dielectric Loss: αd Lossy dielectric ⇒ complex permittivity ⇒ complex wavenumber k σ εε= − j c ω σ k=ω µε = kk µε = µε(1 − j tan δ ) =−−εε′jj ′′ c00 rrc rr d ω =εε′ − ′′ k= k′ − jk ′′ ccj εc′′ =εc′ 1 − j εc′ =εδ′ (1 − j tan ) Note: kk′ = Re{ } cd =εε0 r (1 − j tan δ ) Note : εεrc′ is denoted as r . (e.g., ε r = 2.1 for Teflon). 3 Dielectric Attenuation for TEM Mode TEM mode: kkz = where kk= 0 µεrr (1− j tan δd ) Assume a small dielectric loss in medium: tanδ << 1 Use 1−zz ≈ 1 − /2 for z<< 1 ⇒≈kk0 µεrr(1 − j( tan δd) / 2) kk′ ≈ 0 µεrr 1 kk′′ ≈ µεtan δ 2 0 rr d 4 Summary of Dielectric Attenuation TEM mode kzd=−=βα jk β =Re(kk) = ′ αd =−=Im(kk) ′′ β≈ k0 µεrr 1 α≈ k µεtan δ d 2 0 rr d k=−= k′ jk ′′ k0 µεrr 1 −j tan δd 5 Dielectric Attenuation for Waveguide Mode An exact general expression for the dielectric attenuation: 22 kzd=−=−βα j kk c k=−= k′ jk ′′ k0 µεrr 1 −j tan δd Remember: The value kc is always real, regardless of whether the waveguide filling material is lossy or not.