Peak Inverse Voltage



Similar documents
The Bridge Rectifier

The Full-Wave Rectifier

The circuit shown on Figure 1 is called the common emitter amplifier circuit. The important subsystems of this circuit are:

Linear Circuits Analysis. Superposition, Thevenin /Norton Equivalent circuits

(6)(2) (-6)(-4) (-4)(6) + (-2)(-3) + (4)(3) + (2)(-3) = = 0

Small-Signal Analysis of BJT Differential Pairs

Physics 110 Spring D Motion Problems: Projectile Motion Their Solutions

Luby s Alg. for Maximal Independent Sets using Pairwise Independence

Heuristic Static Load-Balancing Algorithm Applied to CESM

The Greedy Method. Introduction. 0/1 Knapsack Problem

Faraday's Law of Induction

This circuit than can be reduced to a planar circuit

Chapter 12 Inductors and AC Circuits

THE METHOD OF LEAST SQUARES THE METHOD OF LEAST SQUARES

NPAR TESTS. One-Sample Chi-Square Test. Cell Specification. Observed Frequencies 1O i 6. Expected Frequencies 1EXP i 6

Chapter 31B - Transient Currents and Inductance

Chapter 6 Inductance, Capacitance, and Mutual Inductance

Compiling for Parallelism & Locality. Dependence Testing in General. Algorithms for Solving the Dependence Problem. Dependence Testing

Quantization Effects in Digital Filters

8.5 UNITARY AND HERMITIAN MATRICES. The conjugate transpose of a complex matrix A, denoted by A*, is given by

n + d + q = 24 and.05n +.1d +.25q = 2 { n + d + q = 24 (3) n + 2d + 5q = 40 (2)

Series Solutions of ODEs 2 the Frobenius method. The basic idea of the Frobenius method is to look for solutions of the form 3

benefit is 2, paid if the policyholder dies within the year, and probability of death within the year is ).

Logical Development Of Vogel s Approximation Method (LD-VAM): An Approach To Find Basic Feasible Solution Of Transportation Problem

SPEE Recommended Evaluation Practice #6 Definition of Decline Curve Parameters Background:

Rotated Ellipses. And Their Intersections With Lines. Mark C. Hendricks, Ph.D. Copyright March 8, 2012

"Research Note" APPLICATION OF CHARGE SIMULATION METHOD TO ELECTRIC FIELD CALCULATION IN THE POWER CABLES *

Hedging Interest-Rate Risk with Duration

1. Measuring association using correlation and regression

Implementation of Deutsch's Algorithm Using Mathcad

Signal Rectification

Laddered Multilevel DC/AC Inverters used in Solar Panel Energy Systems

NOTE: The Flatpak version has the same pinouts (Connection Diagram) as the Dual In-Line Package. *MR for LS160A and LS161A *SR for LS162A and LS163A

University Physics AI No. 11 Kinetic Theory

Comparison of Control Strategies for Shunt Active Power Filter under Different Load Conditions

Clarify Outline. Installation

Section 5.4 Annuities, Present Value, and Amortization

Figure 1. Inventory Level vs. Time - EOQ Problem

Internet topology dynamics in ten minutes

Laws of Electromagnetism

Fuzzy Set Approach To Asymmetrical Load Balancing In Distribution Networks

Hollinger Canadian Publishing Holdings Co. ( HCPH ) proceeding under the Companies Creditors Arrangement Act ( CCAA )

PHYSICS LAB #2 Passive Low-pass and High-pass Filter Circuits and Integrator and Differentiator Circuits

Efficient Project Portfolio as a tool for Enterprise Risk Management

A Probabilistic Theory of Coherence

Logistic Regression. Lecture 4: More classifiers and classes. Logistic regression. Adaboost. Optimization. Multiple class classification

Solution: Let i = 10% and d = 5%. By definition, the respective forces of interest on funds A and B are. i 1 + it. S A (t) = d (1 dt) 2 1. = d 1 dt.

Forecasting the Demand of Emergency Supplies: Based on the CBR Theory and BP Neural Network

7.5. Present Value of an Annuity. Investigate

v a 1 b 1 i, a 2 b 2 i,..., a n b n i.

Lecture 3: Annuity. Study annuities whose payments form a geometric progression or a arithmetic progression.

Project Networks With Mixed-Time Constraints

1 Example 1: Axis-aligned rectangles

Inter-Ing INTERDISCIPLINARITY IN ENGINEERING SCIENTIFIC INTERNATIONAL CONFERENCE, TG. MUREŞ ROMÂNIA, November 2007.

Rate Monotonic (RM) Disadvantages of cyclic. TDDB47 Real Time Systems. Lecture 2: RM & EDF. Priority-based scheduling. States of a process

Feature selection for intrusion detection. Slobodan Petrović NISlab, Gjøvik University College

CHAPTER 5 RELATIONSHIPS BETWEEN QUANTITATIVE VARIABLES

Brigid Mullany, Ph.D University of North Carolina, Charlotte

FINANCIAL MATHEMATICS. A Practical Guide for Actuaries. and other Business Professionals

L10: Linear discriminants analysis

Lecture 3: Force of Interest, Real Interest Rate, Annuity

Module 2. AC to DC Converters. Version 2 EE IIT, Kharagpur 1

Finite Math Chapter 10: Study Guide and Solution to Problems

RELIABILITY, RISK AND AVAILABILITY ANLYSIS OF A CONTAINER GANTRY CRANE ABSTRACT

Dynamic Routing in Self-Healing MPLS Networks

CHOLESTEROL REFERENCE METHOD LABORATORY NETWORK. Sample Stability Protocol

s-domain Circuit Analysis

Using Series to Analyze Financial Situations: Present Value

Equivalent Circuits and Transfer Functions

14.74 Lecture 5: Health (2)

Lecture 2: Single Layer Perceptrons Kevin Swingler

Vectors. Vector Multiplication

Accident analysis: The role of liability rules pecuniary losses.

Calculating the high frequency transmission line parameters of power cables

Optimal outpatient appointment scheduling

Staff Paper. Farm Savings Accounts: Examining Income Variability, Eligibility, and Benefits. Brent Gloy, Eddy LaDue, and Charles Cuykendall

Analysis and Modeling of Magnetic Coupling

How Sets of Coherent Probabilities May Serve as Models for Degrees of Incoherence

Analysis and Modeling of Buck Converter in Discontinuous-Output-Inductor-Current Mode Operation *

Assurant Employee Benefits City of Frisco Dental DHMO & Dental PPO

Section C2: BJT Structure and Operational Modes

STANDING WAVE TUBE TECHNIQUES FOR MEASURING THE NORMAL INCIDENCE ABSORPTION COEFFICIENT: COMPARISON OF DIFFERENT EXPERIMENTAL SETUPS.

The Development of Web Log Mining Based on Improve-K-Means Clustering Analysis

Production. 2. Y is closed A set is closed if it contains its boundary. We need this for the solution existence in the profit maximization problem.

Texas Instruments 30X IIS Calculator

Support Vector Machines

Transport-Problem-Based Algorithm fordynamicload Balancing in Distributed LogicSimulation

Lecture 2 Sequence Alignment. Burr Settles IBS Summer Research Program 2008 bsettles@cs.wisc.edu

Chapter 4 ECONOMIC DISPATCH AND UNIT COMMITMENT

The OC Curve of Attribute Acceptance Plans

) of the Cell class is created containing information about events associated with the cell. Events are added to the Cell instance

Effect of a spectrum of relaxation times on the capillary thinning of a filament of elastic liquid

Extending Probabilistic Dynamic Epistemic Logic

Problem Set 3. a) We are asked how people will react, if the interest rate i on bonds is negative.

Transcription:

9/13/2005 Peak Inerse Voltage.doc 1/6 Peak Inerse Voltage Q: I m so confused! The brdge rectfer and the fullwae rectfer both prode full-wae rectfcaton. Yet, the brdge rectfer use 4 juncton dodes, whereas the full-wae rectfer only uses 2. Why would we eer want to use the brdge rectfer? A: Frst, a slght confesson the results we dered for the brdge and full-wae rectfers are not precsely correct! Recall that we used the juncton dode CV model to determne the transfer functon of each rectfer crcut. The problem s that the CV model does not predct juncton dode breakdown! If the source oltage becomes too large, the juncton dodes can n fact breakdown but the transfer functons we dered do not reflect ths fact! Q: You mean that we must rework our analyss and fnd new transfer functons!? Jm tles The Un. of Kansas ept. of EEC

9/13/2005 Peak Inerse Voltage.doc 2/6 A: Fortunately no. Breakdown s an undesrable mode for crcut rectfcaton. Our job as engneers s to desgn a rectfer that aods t that why the brdge rectfer s helpful! To see why, consder the oltage across a reersed based juncton dode n each of our rectfer crcut desgns. Recall that the oltage across a reerse based deal dode n the full-wae rectfer desgn was: 2 = 2 so that the oltage across the juncton dode s approxmately: = + 0.7 = 2 + 0.7 Now, assumng that the source oltage s a sne wae = Asnωt, we fnd that dode oltage s at t most negate (.e., breakdown danger!) when the source oltage s at ts maxmum alue A. I.E.,: = 2A + 07. mn Of course, the largest juncton dode oltage occurs when n forward bas: = 07V. max Jm tles The Un. of Kansas ept. of EEC

9/13/2005 Peak Inerse Voltage.doc 3/6 A (t) 0.7 t 2A + 07. (t) Note that ths mnmum dode oltage s ery negate, wth an absolute alue ( mn = 2A 07. ) nearly twce as large as the source magntude A. We call the absolute alue of the mnmum dode oltage the Peak Inerse Voltage (PIV): mn PIV = Note that ths alue s dependent on both the rectfer desgn and the magntude of the source oltage. Q: o, why do we need to determne PIV? I m not sure I see what dfference ths alue makes. Jm tles The Un. of Kansas ept. of EEC

9/13/2005 Peak Inerse Voltage.doc 4/6 A: The Peak Inerse Voltage answers one mportant queston wll the juncton dodes n our rectfer breakdown? If the PIV s less than the Zener breakdown oltage of our rectfer dodes (.e., f PIV < VZK ), then we know that our juncton dodes wll reman n ether forward or reerse bas for all tme t. The rectfer wll operate properly! Howeer, f the PIV s greater than the Zener breakdown oltage of our rectfer dodes (.e., f PIV > VZK ), then we know that our juncton dodes wll breakdown for at least some small amount of tme t. The rectfer wll NOT operate properly! Q: o what do we do f PIV s greater than V ZK? How do we fx ths problem? A: We hae two possble solutons: 1. Use juncton dodes wth larger alues of V ZK (f they exst!). 2. Use the brdge rectfer desgn. Q: The brdge rectfer! How would that sole our breakdown problem? Jm tles The Un. of Kansas ept. of EEC

9/13/2005 Peak Inerse Voltage.doc 5/6 A: To see how a brdge rectfer can be useful, let s determne ts Peak Inerse Voltage PIV. Frst, we recall that the oltage across the reerse based deal dodes was: = so that the oltage across the juncton dode s approxmately: = + 0.7 = + 0.7 Now, assumng that the source oltage s a sne wae = Asnωt, we fnd that dode oltage s at t most negate (.e., breakdown danger!) when the source oltage s at ts maxmum alue A. I.E.,: = A + 07. mn Of course, the largest juncton dode oltage occurs when n forward bas: = 07V. max Jm tles The Un. of Kansas ept. of EEC

9/13/2005 Peak Inerse Voltage.doc 6/6 A (t) 0.7 t A + 07. (t) Note that ths mnmum dode oltage s ery negate, wth an absolute alue ( mn = A 07. ), approxmately equal to the alue of the source magntude A. Thus, the PIV for a brdge rectfer wth a snusodal source oltage s: PIV = A 07. Note that ths brdge rectfer alue s approxmately half the PIV we determned for the full-wae rectfer desgn! Thus, the source oltage (and the output C component) of a brdge rectfer can be twce that of the full-wae rectfer desgn ths s why the brdge rectfer s a ery useful rectfer desgn! Jm tles The Un. of Kansas ept. of EEC