Calculation of Inrush Current During Capacitor Bank Energization

Similar documents
ELE B7 Power Systems Engineering. Symmetrical Components

Name of the Student:

Time-Domain Representations of LTI Systems

LC Oscillations. di Q. Kirchoff s loop rule /27/2018 1

Chapter 9 - CD companion 1. A Generic Implementation; The Common-Merge Amplifier. 1 τ is. ω ch. τ io

Live Line Measuring the Parameters of 220 kv Transmission Lines with Mutual Inductance in Hainan Power Grid

8. СОВЕТУВАЊЕ. Охрид, септември ANALYSIS OF NO LOAD APPARENT POWER AND FREQUENCY SPECTRUM OF MAGNETIZING CURRENT FOR DIFFERENT CORE TYPES

The Scattering Matrix

EE692 Applied EM- FDTD Method One-Dimensional Transmission Lines Notes- Lecture 4

Section 5.5. Infinite Series: The Ratio Test

ADVANCED DIGITAL SIGNAL PROCESSING

EXPERIMENT OF SIMPLE VIBRATION

mx bx kx F t. dt IR I LI V t, Q LQ RQ V t,

Sinusoidal Steady-state Analysis

Appendix: The Laplace Transform

62. Power series Definition 16. (Power series) Given a sequence {c n }, the series. c n x n = c 0 + c 1 x + c 2 x 2 + c 3 x 3 +

Chapter 4. Fourier Series

Chapter 7: The z-transform. Chih-Wei Liu

Z - Transform. It offers the techniques for digital filter design and frequency analysis of digital signals.

Response Analysis on Nonuniform Transmission Line

1 6 = 1 6 = + Factorials and Euler s Gamma function

Exmple Questions for the Examination for 4041 OPTICAL COMMUNICATION ENGINEERING

Seunghee Ye Ma 8: Week 5 Oct 28

Chapter 11 Output Analysis for a Single Model. Banks, Carson, Nelson & Nicol Discrete-Event System Simulation

FREE VIBRATION RESPONSE OF A SYSTEM WITH COULOMB DAMPING

Physics 116A Solutions to Homework Set #1 Winter Boas, problem Use equation 1.8 to find a fraction describing

Sinusoidal stimulus. Sin in Sin at every node! Phasors. We are going to analyze circuits for a single sinusoid at a time which we are going to write:

Unit 5 - Week 4. Week 4: Assignment. Course outline. Announcements Course Forum Progress Mentor

Solutions of Chapter 5 Part 1/2

CMOS. Dynamic Logic Circuits. Chapter 9. Digital Integrated Circuits Analysis and Design

Calculation of Fundamental Impedance Characteristic of a TCSC using a Normalised Model

CS322: Network Analysis. Problem Set 2 - Fall 2009

Mathematics 116 HWK 21 Solutions 8.2 p580

EE 505. Lecture 29. ADC Design. Oversampled

FREE VIBRATIONS OF SIMPLY SUPPORTED BEAMS USING FOURIER SERIES

UNIVERSITY OF CALIFORNIA, BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences

Simplified Approach for Synthesizing Frequency Dependent Network Equivalents Including Dynamic Behaviors of Large Power Transmission Systems

Analysis of five-parameter Viscoelastic model under Dynamic Loading

COMM 602: Digital Signal Processing

Analysis of MOS Capacitor Loaded Annular Ring MICROSTRIP Antenna

Chapter 4 : Laplace Transform

SPEC/4/PHYSI/SPM/ENG/TZ0/XX PHYSICS PAPER 1 SPECIMEN PAPER. 45 minutes INSTRUCTIONS TO CANDIDATES

Proceedings of the 2nd International Conference on Computer Science and Electronics Engineering (ICCSEE 2013)

Q-BINOMIALS AND THE GREATEST COMMON DIVISOR. Keith R. Slavin 8474 SW Chevy Place, Beaverton, Oregon 97008, USA.

CSI 2101 Discrete Structures Winter Homework Assignment #4 (100 points, weight 5%) Due: Thursday, April 5, at 1:00pm (in lecture)

GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL OF ELECTRICAL AND COMPUTER ENGINEERING

1.3 Convergence Theorems of Fourier Series. k k k k. N N k 1. With this in mind, we state (without proof) the convergence of Fourier series.

Are the following series absolutely convergent? n=1. n 3. n=1 n. ( 1) n. n=1 n=1

ECONOMIC OPERATION OF POWER SYSTEMS

Linear Associator Linear Layer

The Phi Power Series

Solution of Linear Constant-Coefficient Difference Equations

Olli Simula T / Chapter 1 3. Olli Simula T / Chapter 1 5

Regenerative Property

Most text will write ordinary derivatives using either Leibniz notation 2 3. y + 5y= e and y y. xx tt t

The optimal online control of the instantaneous power and the multiphase source s current

Fundamental Concepts: Surfaces and Curves

Comparison of High Frequency Detailed Generator Models for Partial Discharge Localization

STPS340U/S/B POWER SCHOTTKY RECTIFIER MAIN PRODUCT CHARACTERISTICS. 3A 40 V Tj (max) 150 C FEATURES AND BENEFITS

ECE 422/522 Power System Operations & Planning/Power Systems Analysis II : 6 - Small Signal Stability

PAPER : IIT-JAM 2010

Introduction to Signals and Systems, Part V: Lecture Summary

REVIEW 1, MATH n=1 is convergent. (b) Determine whether a n is convergent.

Bipolar Junction Transistors

Quiz. Use either the RATIO or ROOT TEST to determine whether the series is convergent or not.

Section A assesses the Units Numerical Analysis 1 and 2 Section B assesses the Unit Mathematics for Applied Mathematics

Math 142, Final Exam. 5/2/11.

1 1 2 = show that: over variables x and y. [2 marks] Write down necessary conditions involving first and second-order partial derivatives for ( x0, y

(b) What is the probability that a particle reaches the upper boundary n before the lower boundary m?

Signal Processing in Mechatronics. Lecture 3, Convolution, Fourier Series and Fourier Transform

EE / EEE SAMPLE STUDY MATERIAL. GATE, IES & PSUs Signal System. Electrical Engineering. Postal Correspondence Course

Chapter 10 Partial Differential Equations and Fourier Series

Butterworth LC Filter Designer

Charge Recycling in MTCMOS Circuits: Concept and Analysis Ehsan Pakbaznia University of Southern California

Chapter 2 Feedback Control Theory Continued

POWER SERIES SOLUTION OF FIRST ORDER MATRIX DIFFERENTIAL EQUATIONS

Matrix Algebra 2.2 THE INVERSE OF A MATRIX Pearson Education, Inc.

Solutions. Number of Problems: 4. None. Use only the prepared sheets for your solutions. Additional paper is available from the supervisors.

LECTURE SERIES WITH NONNEGATIVE TERMS (II). SERIES WITH ARBITRARY TERMS

ChE 471 Lecture 10 Fall 2005 SAFE OPERATION OF TUBULAR (PFR) ADIABATIC REACTORS

You may work in pairs or purely individually for this assignment.

MATH 10550, EXAM 3 SOLUTIONS

Integer Linear Programming

CUMULATIVE DAMAGE ESTIMATION USING WAVELET TRANSFORM OF STRUCTURAL RESPONSE

Generating Functions for Laguerre Type Polynomials. Group Theoretic method

The state space model needs 5 parameters, so it is not as convenient to use in this control study.

Development of a Methodology for Evaluating the Reliability of Transformer Differential Protection Function Based on Monte Carlo Method

FIR Filter Design: Part II

The Z-Transform. (t-t 0 ) Figure 1: Simplified graph of an impulse function. For an impulse, it can be shown that (1)

EDEXCEL NATIONAL CERTIFICATE UNIT 4 MATHEMATICS FOR TECHNICIANS OUTCOME 4 - CALCULUS

3. Z Transform. Recall that the Fourier transform (FT) of a DT signal xn [ ] is ( ) [ ] = In order for the FT to exist in the finite magnitude sense,

MAS160: Signals, Systems & Information for Media Technology. Problem Set 5. DUE: November 3, (a) Plot of u[n] (b) Plot of x[n]=(0.

*X203/701* X203/701. APPLIED MATHEMATICS ADVANCED HIGHER Numerical Analysis. Read carefully

EE 505. Lecture 28. ADC Design SAR

2. Fourier Series, Fourier Integrals and Fourier Transforms

Ray Optics Theory and Mode Theory. Dr. Mohammad Faisal Dept. of EEE, BUET

Stability Analysis and Bifurcation Control of Hysteresis Current Controlled Ćuk Converter Using Filippov s Method

Realization of a Smart Electrolytic Capacitor Circuit

A PROCEDURE TO MODIFY THE FREQUENCY AND ENVELOPE CHARACTERISTICS OF EMPIRICAL GREEN'S FUNCTION. Lin LU 1 SUMMARY

Math 116 Practice for Exam 3

Transcription:

Protectio of lectrical Networks hristophe Preve opyright 0 006, IST td. Appedix B alculatio of Irush urret Durig apacitor Bak ergizatio Fixed bak The equivalet stream etwork sigle-phase diagram durig eergizatio of the fixed bak is show i Figure B-. (t) (): t sigle-phase voltage : stream etwork iductace : iductace of the coectio likig the switchig device to the capacitor bak Figure B-: equivalet diagram durig fixed bak eergizatio

494 Protectio of lectrical Networks We shall demostrate that the frequecy of the trasiet curret occurrig o eergizatio is very high (see sectio 0.6., example ; f0, 58 Hz ). This results i justificatio of eglect of the etwork resistace i relatio to the iductace: R f0, sice f0 50 Hz. Similarily, the resistace of the coectio likig the switchig device to the capacitor is egligible. The etwork frequecy (50 Hz) is egligible i relatio to the trasiet curret frequecy. We might therefore cosider that we have a voltage step throughout the duratio of the trasiet curret. The value of the step, at worst, is the peak value of the siusoidal voltage: U U : phase-to-phase voltage The curret it is determied by the followig differetial equatio: t di dt i d where: () t 0 for t 0 () t ˆ for t 0 We shall solve this equatio usig aplace trasforms. As a aplace trasform, the differetial equatio becomes: ˆ V t 0 0 s I s i t I s s s s The curret is zero before eergizatio ad it is assumed that the voltage at the capacitor termials is zero (worst case). Hece: it 0 0 ad V t 0 0

Appedix B 495 ˆ s s thus givig us: s Is Is hece: I s ˆ ˆ s s s s et us take: I s s Usig the aplace trasform tables, we ca deduce it : it ˆ si t it U si t The maximum peak irush curret is thus: Iˆ rush U A ad its frequecy: f 0 Switched steps bak The equivalet sigle-phase diagram durig switched steps bak eergizatio is show i Figure B-.

496 Protectio of lectrical Networks + U : stream etwork iductace : iductace of the coectio likig the switchig device to the bak Figure B-: equivalet diagram durig switched steps bak eergizatio The peak irush curret Irush is maximum whe baks are i service ad the th oe is eergized. The baks i service off load ito the bak that has just bee eergized. The stream iductace is very high i relatio to iductace (see sectio 0.6., example : 85 H ad example :.5 H). The curret splied by the stream part (etwork) is therefore eglected. It is assumed that, at worst, o eergizatio the voltage at the termials of U V t 0. each capacitor is ˆ The equivalet diagram is thus show i Figure B-. The diagram comprises parallel-coected braches with a impedace of Z j. j The equivalet impedace is therefore: Z eq Z j j

Appedix B 497 + : iitial voltage coditio at the capacitor termials Figure B- The diagram thus becomes that of Figure B-4. Figure B-4

498 Protectio of lectrical Networks We have two series-coected iductaces: We have two series-coected capacitaces: The equivalet diagram is thus that i Figure B-5. Figure B-5 The equivalet diagram i Figure B-5 is the same as that of a fixed bak. If we re-use the formula for a fixed bak, we immediately obtai:

Appedix B 499 U I rush ˆ U I rush ˆ f