ELEC-E8409 HIGH VOLTAGE ENGINEERING

Slides:



Advertisements
Similar presentations
Note 2 Transmission Lines (Time Domain)
Advertisements

Twisted Pairs Another way to reduce cross-talk is by means of a twisted pair of wires. A twisted pair of wires will be modeled as a cascade of alternating.
Characteristic Impedance Contnd. Air Dielectric Parallel Line Coaxial Cable Where: D = spacings between centres of the conductors r = conductor radius.
Co-Axial Cable Analysis. Construction Details Question 1 What is the fundamental equation relating the magnetic field surrounding a conductor and the.
EKT241 – ELECTROMAGNETICS THEORY
Physics for Scientists and Engineers II, Summer Semester Lecture 20: July 10 th 2009 Physics for Scientists and Engineers II.
Frequency dependent Measurement and theoretical Prediction of Characteristic Parameters of Vacuum Cable Micro-Striplines - Risetime of a typical ATLAS.
KAVOSHCOM RF Communication Circuits Lecture 1: Transmission Lines.
CSE245: Computer-Aided Circuit Simulation and Verification Lecture Note 2: State Equations Prof. Chung-Kuan Cheng 1.
Series-Parallel Combinations of Inductance and Capacitance
UCSD CSE245 Notes -- Spring 2006 CSE245: Computer-Aided Circuit Simulation and Verification Lecture Notes Spring 2006 Prof. Chung-Kuan Cheng.
Traveling Wave Transient Overvoltages. 1.Introduction Transient Phenomenon : –Aperiodic function of time –Short duration Example :Voltage & Current Surge.
Lecture - 4 Inductance and capacitance equivalent circuits
Magnetics Design Primary Constraints:
General Licensing Class G5A – G5C Electrical Principles Your organization and dates here.
Advanced Microwave Measurements
CSE245: Computer-Aided Circuit Simulation and Verification Lecture Note 2: State Equations Prof. Chung-Kuan Cheng.
Lecture 4.  1.5 The terminated lossless transmission line What is a voltage reflection coefficient? Assume an incident wave ( ) generated from a source.
Motional EMF This is the emf induced in a conductor moving through a magnetic field. Examples on sheet 10 To change the magnetic flux we can change: 1.the.
Transmission Lines No. 1  Seattle Pacific University Transmission Lines Kevin Bolding Electrical Engineering Seattle Pacific University.
Fundamentals of Electric Circuit Analysis, by Clayton Paul Copyright 2000 © John Wiley & Sons. Inc. All rights reserved. Figure 5.1 A parallel-plate capacitor.
Fundamentals of Electric Circuits Chapter 13 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
L1-1 ELECTROMAGNETICS AND APPLICATIONS Lecture 8 TEM Transmission Lines Luca Daniel.
11/22/2004EE 42 fall 2004 lecture 351 Lecture #35: data transfer Last lecture: –Communications synchronous / asynchronous –Buses This lecture –Transmission.
MAGNETICALLY COUPLED NETWORKS
Impedance Measurements on a PCB
Electromagnetic Induction. Motion of a magnet in a coil or loop creates (induces) voltage If coil is connected to complete circuit, current flows Relative.
CSE245: Computer-Aided Circuit Simulation and Verification Lecture Note 2: State Equations Spring 2010 Prof. Chung-Kuan Cheng.
ECE Networks & Systems Jose E. Schutt-Aine
Level 2 Electromagnetism Laboratory Experiment
Magnetically coupled circuits
Electrical Engineering
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons Figure 2.1 (p. 50) Voltage and current definitions and equivalent.
ENE 490 Applied Communication Systems
Lecture 3.
Chapter 2 Transmission Line Theory (2.1 ~ 2.5) 전자파연구실 1.
Electronic Circuits, Tenth Edition James W. Nilsson | Susan A. Riedel Copyright ©2015, 2008, 2005 by Pearson Education, Inc. All rights reserved. Figure.
Chapter 2 Overview 1.
Crosstalk Crosstalk is the electromagnetic coupling among conductors that are close to each other. Crosstalk is an EMC concern because it deals with the.
Lab2: Smith Chart And Matching
Circuits II EE221 Unit 10 Instructor: Kevin D. Donohue
LAPLACE TRANSFORM AS AN USEFUL TOOL IN TRANSIENT STATE ANALYSIS
Analysis of the Amplitude and Frequencies of the Voltage Magnification Transients in Distribution Networks due to Capacitor Switching Mohamed Saied Electrical.
How does a signal go through the cable
Network Analysis and Synthesis
ECE 3301 General Electrical Engineering
ELEC-E8409 HIGH VOLTAGE ENGINEERING
Characteristic Impedance Contnd.
ELEC-E8409 HIGH VOLTAGE ENGINEERING
Non-ideal property – crosstalk
EE758 Numerical Techniques in Electromagnetics Lecture 3
WELCOME.
transmission line models
Last lecture Motional EMF
CHAPTER 4 AC Network Analysis.
I made an impedance matching circuit but forgot which impedance was originally matched. Find the unknown load impedance. What is the impedance that the.
Power transmission Energy is lost in transmission lines
Exercise 8 Power systems.
Lecture 14. Diagnostic equipment of the accelerators
ELL100: INTRODUCTION TO ELECTRICAL ENGG.
Electromagnetics II Unit 1:Basics of Transmission Lines
Exercise Session 2 Power systems.
Midterm Solutions Source Transformations
Applied Electromagnetic Waves Notes 6 Transmission Lines (Time Domain)
ENE 428 Microwave Engineering
Microwave Engineering
7e Applied EM by Ulaby and Ravaioli
Power System Analysis (EELE 4351)
Exercise Session 11 Power systems.
4th Week Seminar Sunryul Kim Antennas & RF Devices Lab.
Presentation transcript:

ELEC-E8409 HIGH VOLTAGE ENGINEERING Exercise 3 ELEC-E8409 HIGH VOLTAGE ENGINEERING

Question 1 A step wave of amplitude u is applied to the open line illustrated in the figure. Study voltage as a function of time at points A, B and C. s m v l Z j / 10 300 450 400 6 = W k 150 40 A B C u .

Transmission coefficient: Reflection coefficient: Ground Bare Conductor Cable Open End Z = 0 Z = 400 Ω Z = 40 Ω Z =∞ τ1 τ2 τ3 τ4 ρ1 ρ2 ρ3 ρ4 A B C (τ2, ρ2): Z1 = 400 Ω, Z2 = 40 Ω (τ1, ρ1): Z1 = 400 Ω, Z2 = 0 (τ4, ρ4): Z1 = 40 Ω, Z2 = ∞ (τ3, ρ3): Z1 = 40 Ω, Z2 = 400 Ω

Propagation of waveform: B C 10 9 8 7 6 t [µs] 5 4 3 2 1 τ2 τ3 ρ1 ρ2 ρ3 ρ4 τ4

Uc 0.96 (7.5µs) Ub 0.78 (7.5µs) 0.66 (5.5µs) 0.66 (6.5µs) 0.36 (3.5µs) 1.2 Ua 0.2 0.4 0.6 0.8 1 1.2 2 3 4 5 6 7 8 9 10 Time [µs] Uc 0.96 (7.5µs) 1.0 Ub 0.8 0.78 (7.5µs) 0.66 (5.5µs) 0.66 (6.5µs) Voltage 0.6 0.36 (3.5µs) 0.4 0.33 (4.5µs) 0.2 0.18 (1.5µs) 0.0 1 2 3 4 5 6 7 8 9 10 Time [µs]

Question 2 A current transformer is linked to a 20-kV bare conductor line. The primary coil inductance is 100 µH. Wave impedance of the line is 500 Ω. A step wave of amplitude 110 kV arrives at the current transformer. Show, using equations and approximate drawings, both of the transformer’s 20-kV terminals against ground and also the voltage between the terminals.

û =110 kV 1 2 L = 100 µH Z = 500 Ω 1 2 Z1 Z2 u2 u1 u12 2û Easy Solution Lecture slides:

Derive the equations using Laplace transformation: 1 2 Z1 Z2 u2 u1 u12 2û Derive the equations using Laplace transformation: Z sL + Z 2û s u1 u1 Laplace Laplace

Derive the equations using Laplace transformation: 1 2 Z1 Z2 u2 u1 u12 2û Derive the equations using Laplace transformation: sL + Z Z 2û s u2 u2 Laplace

Derive the equations using Laplace transformation: 1 2 Z1 Z2 u2 u1 u12 2û Derive the equations using Laplace transformation: Z sL 2û s u12 u12 Laplace

250 Z1 Z2 u2 u1 u12 2û 200 150 Voltage [kV] 100 50 0.05 0.1 0.15 0.2 0.25 0.3 0.35 Time [µs]

Question 3 An overhead line receives a square impulse of amplitude 100 kV and length 2 km at point A. Point A is connected to a spark gap parallel with a 0.01 µF capacitor. The inception voltage of the gap is 50 kV. Draw the reflecting waveform at point A and define the waveform parameters.

Equivalent Circuit s = 2000 m û = 100 kV Z1 = 500 Ω Z2 = 500 Ω A C = 0.01 µF A Z1 Z2 u2 2û Equivalent Circuit

Inception time (moment of ignition) Inception voltage of spark gap = 50 kV: Inception time (moment of ignition) Duration of impulse (v = speed of light c)

U1 U2 Voltage [kV] t [µs] Ur = U2 – U1 120 100 80 60 40 20 1 2 3 4 5 6 U2 = 100(1 – e -t/τ ) 60 50 kV U1 40 U2 20 t = 1.73 µs Voltage [kV] t [µs] 1 2 3 4 5 6 7 8 9 10 -20 -40 -60 -80 Ur = U2 – U1 -100 -120

Derive the equations using Laplace transformation: Z1 Z2 u2 2û Derive the equations using Laplace transformation: A Z sC 1 2û s Z u2 u1 Laplace