ELEC 425 Interference Control in Electronics Lecture 1(c) Review of Decibels & Decibel Arithmetic

Similar documents
Fundamentals of Engineering Exam Review Electromagnetic Physics

ELEC 202 Electric Circuit Analysis II Lecture 10(a) Complex Arithmetic and Rectangular/Polar Forms

db: Units & Calculations

Determining Characteristic Impedance and Velocity of Propagation by Measuring the Distributed Capacitance and Inductance of a Line

EE 205 Dr. A. Zidouri. Electric Circuits II. Two-Port Circuits Two-Port Parameters. Lecture #42

Module 3 : Sequence Components and Fault Analysis

EELE 3332 Electromagnetic II Chapter 11. Transmission Lines. Islamic University of Gaza Electrical Engineering Department Dr.

Lecture Outline. Attenuation Coefficient and Phase Constant Characteristic Impedance, Z 0 Special Cases of Transmission Lines

ECE 5260 Microwave Engineering University of Virginia. Some Background: Circuit and Field Quantities and their Relations

Use of the decibel and the neper

Pulses in transmission lines

Chapter 10 AC Analysis Using Phasors

Lecture Outline. Scattering at an Impedance Discontinuity Power on a Transmission Line Voltage Standing Wave Ratio (VSWR) 8/10/2018

ECE 3300 Standing Waves

Review Quantitative Aspects of Networking. Decibels, Power, and Waves John Marsh

ANTENNAS and MICROWAVES ENGINEERING (650427)

1.3 Sinusoidal Steady State

TC 412 Microwave Communications. Lecture 6 Transmission lines problems and microstrip lines

Thevenin equivalent circuits

Microwave Circuit Design I

Lecture 12. Microwave Networks and Scattering Parameters

Pulses in transmission lines

PHY3128 / PHYM203 (Electronics / Instrumentation) Transmission Lines

ELEC Introduction to power and energy systems. The per unit system. Thierry Van Cutsem

Single-Time-Constant (STC) Circuits This lecture is given as a background that will be needed to determine the frequency response of the amplifiers.

Transformer. Transformer comprises two or more windings coupled by a common magnetic circuit (M.C.).

Chapter 5 Steady-State Sinusoidal Analysis

Name. Section. Short Answer Questions. 1. (20 Pts) 2. (10 Pts) 3. (5 Pts) 4. (10 Pts) 5. (10 Pts) Regular Questions. 6. (25 Pts) 7.

and Ee = E ; 0 they are separated by a dielectric material having u = io-s S/m, µ, = µ, 0

Contents. Transmission Lines The Smith Chart Vector Network Analyser (VNA) ü structure ü calibration ü operation. Measurements

Study Notes on Network Theorems for GATE 2017

Dr. Vahid Nayyeri. Microwave Circuits Design

Contents. Transmission Lines The Smith Chart Vector Network Analyser (VNA) ü structure ü calibration ü operation. Measurements

Lecture Outline. Shorted line (Z L = 0) Open circuit line (Z L = ) Matched line (Z L = Z 0 ) 9/28/2017. EE 4347 Applied Electromagnetics.

Impedance and Admittance Parameters

Lecture (5) Power Factor,threephase circuits, and Per Unit Calculations

TECHNO INDIA BATANAGAR

If an Ohm is the place where a Volt lives, Watt is db said for current? Does it live in a bun?

ECE 604, Lecture 13. October 16, 2018

2. The following diagram illustrates that voltage represents what physical dimension?

Wave Phenomena Physics 15c. Lecture 8 LC Transmission Line Wave Reflection

One-Port Networks. One-Port. Network

How to measure complex impedance at high frequencies where phase measurement is unreliable.

Modeling of Overhead Power Lines for Broadband PLC Applications.

Contents. ! Transmission Lines! The Smith Chart! Vector Network Analyser (VNA) ! Measurements. ! structure! calibration! operation

Statistical modelling of TV interference for shared-spectrum devices

Experiment #6. Thevenin Equivalent Circuits and Power Transfer

Assignment 3 ELEC 312/Winter 12 R.Raut, Ph.D.

6.976 High Speed Communication Circuits and Systems Lecture 2 Transmission Lines

Electric Circuit Theory

Lecture 6: Impedance (frequency dependent. resistance in the s-world), Admittance (frequency. dependent conductance in the s-world), and

A two-port network is an electrical network with two separate ports

INTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012

Electrical Circuits I Lecture 8

TRANSMISSION LINES AND MATCHING

Direct Current (DC): In a DC circuit the current and voltage are constant as a function of time. Power (P): Rate of doing work P = dw/dt units = Watts

EE221 - Practice for the Midterm Exam

Module 2 : Transmission Lines. Lecture 1 : Transmission Lines in Practice. Objectives. In this course you will learn the following

ESE319 Introduction to Microelectronics Bode Plot Review High Frequency BJT Model

8.1 Circuit Parameters

To investigate further the series LCR circuit, especially around the point of minimum impedance. 1 Electricity & Electronics Constructor EEC470

Lecture Outline 9/27/2017. EE 4347 Applied Electromagnetics. Topic 4a

Basic Electronics. Introductory Lecture Course for. Technology and Instrumentation in Particle Physics Chicago, Illinois June 9-14, 2011

ELG4125: Power Transmission Lines Steady State Operation

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Statistical Physics I Spring Term 2013

Circuit Representation of TL s A uniform TL may be modeled by the following circuit representation:

ELECTRONICS IA 2017 SCHEME

Lecture 17 Date:

Chapter 1W Basic Electromagnetic Concepts

4.10 Unbalanced fault analysis using Z BUS matrix:

Physics 7B-1 (A/B) Professor Cebra. Winter 2010 Lecture 2. Simple Circuits. Slide 1 of 20

NR/RR. Set No. 2 CODE NO: NR/RR210204

Symmetrical Components. References

Lecture 11: J-FET and MOSFET

Thevenin S And Norton S Theorems

Keysight Technologies Fundamentals of RF and Microwave Power Measurements (Part 3) Application Note

Lecture 19 Date:

Ch 8. Three-phase systems

Lowpass L Matching Network Designer

SOME USEFUL NETWORK THEOREMS

Accelerated Taylor State Plumes in SSX

Chapter 11: WinTDR Algorithms

Chapter 5 Objectives

Electromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance

ECE 107: Electromagnetism

Reflection & Transmission

S.E. Sem. III [EXTC] Circuits and Transmission Lines

MCE603: Interfacing and Control of Mechatronic Systems. Chapter 1: Impedance Analysis for Electromechanical Interfacing

Numerical Solution of BLT Equation for Inhomogeneous Transmission Line Networks

CIRCUITS AND ELECTRONICS. Energy and Power

AC Circuits III. Physics 2415 Lecture 24. Michael Fowler, UVa

Physics 401 Classical Physics Laboratory. Experiment 5. Transients and Oscillations in RLC Circuits. I. Introduction II. Theory...

AN80xx/AN80xxM Series

Transducer Control Algorithms

Short Wire Antennas: A Simplified Approach Part I: Scaling Arguments. Dan Dobkin version 1.0 July 8, 2005

No prep assignment to do, but here are four questions anyway.

Chapter 24 Photonics Question 1 Question 2 Question 3 Question 4 Question 5

Two-Port Networks Admittance Parameters CHAPTER16 THE LEARNING GOALS FOR THIS CHAPTER ARE THAT STUDENTS SHOULD BE ABLE TO:

Structure of Biological Materials

Prepare for this experiment!

Transcription:

Dr. Gregory J. Mazzaro Fall 2017 ELEC 425 Interference Control in Electronics Lecture 1(c) Review of Decibels & Decibel rithmetic THE CITDEL, THE MILITRY COLLEGE OF SOUTH CROLIN 171 Moultrie Street, Charleston, SC 29409

2 Logarithms x N b log N x where N = positive number ( linear value ) b b = the base of the logarithm x = the exponent of the logarithm -- a way to easily write/compare numbers that are very large and/or very small, simultaneously -- an alternative to scientific notation using b = 10 ( base-10 ) N x 0.000001 6 0.001 3 1 0 1, 000 3 1,000,000 6 Typical electric fields range from 1 m/m to 200 /m 8 orders of magnitude. The decibel scale compresses this data to a narrower range of numbers.

Gain & Decibels Gain () refers to the ratio of put-to-input voltage, current, field, power, etc. p v in p v 20log10 p 10log10 in in in in in p W W in p Decibels are a convenient format used to express very high/low gain (up/down to very high/low values of voltage, field, power). in p,1 p,2 p p,1 p,2 p p,1 p,2 3

Gain (/) Gain () 4 Decibels: The decibel scale is a logarithmic log N x scale that uses base b = 10. 10 By convention, gain in decibels is v v 12 6 20log 10 v v 10log 10 p p v 3 v 10 60 2 10 40 10 20 2 6 1 0 0.5 6 0.1 20 2 10 40 3 10 60

ower (m) ower (mw) 5 Decibels: m The decibel scale is a logarithmic log N x scale that uses base b = 10. 10 By convention, power in decibels (referenced to 1 milliwatt) is 10 20 m 1 2 mw 3m 10log 10 1 mw W m 3 10 60 10 40 1 30 0.1 20 0.01 10 3 10 6 10 9 10 12 10 0 30 60 90 30

Field (m/m) Field (m/m) 6 Decibels: m/m The decibel scale is a logarithmic log N x scale that uses base b = 10. 10 By convention, electric field in decibels (referenced to 1 microvolt per meter) is E μ/m E 1 2μ/m 6 μ/m E 20log 10 1μ m E μ/m 3 E μ/m 10 60 2 10 40 10 20 2 6 1 0 0.5 6 0.1 20 2 10 40 3 10 60

Decibels: Circuits & Gain I in I in R 2 in in R 2 L v i p I I in in in v 20log10 in I i 20log10 Iin p 10log10 in where in,, I in, I are assumed to be RMS values. 7

Decibels: oltage, Current, ower, Field I in I I I 20log 1 m m 10 20log 1μ μ 10 I 20log 1 m m 10 I 20log 1μ μ 10 E E E 20log 1 m/m m/m 10 E 20log 1μ/m μ/m 10 10log 1 mw mw 10 8 where, I, E are assumed to be RMS values.

Examples: Decibel Conversions Express the ratios of the following quantities in decibels: (a) a power of 20 W to a power of 1 mw (b) a current of 2 m RMS to a current of 0.5 RMS Convert the following quantities to the specified decibel units: (c) 20 m/m to m/m (d) 300 mw to m 9

Dr. Gregory J. Mazzaro Fall 2017 ELEC 425 Interference Control in Electronics Lecture 1(d) Cable Losses & High-Frequency Signal Sources THE CITDEL, THE MILITRY COLLEGE OF SOUTH CROLIN 171 Moultrie Street, Charleston, SC 29409

Transmission-Line Theory complete mathematical model for the transmission-line circuit yields (in Section 1.5.1) 2 d 2 dz 0 2 j r jl g jc The general solution to this wave equation is z e e, I z I e I e z z z z 0 0 0 0 which is a pair of waves: one travels from source to measurer ; the other travels from measurer to source. e z 0 The ratio of voltage-to-current for one of the waves is the characteristic impedance, Z C e z 0 Z C r jl I g jc 0 0 12

Circuit Models for Instruments t a particular frequency (or within a narrow band of frequencies) 13

Matched System (50 W) system is matched when the Thevenin impedance of the source, the characteristic impedance, and the Thevenin impedance of the measurer are equal. Our industry standard is 50 W. When all impedances are matched, the solution is z e, I z I e For a mismatched load/cable, the signal z z 0 0 which is one wave, traveling from source to measurer. source put may be determined using e z 0 14

Cable (ower) Loss The system is assumed to be matched (usually to 50 W). z = 0 z = L When all impedances are matched, the solution is z e, I z I e, j z z 0 0 which carries the time-average power 2 1 1 0 2 z avg z Re z I z e coszc 2 2 Z C attenuation with distance into the cable z Cable loss (in ) is calculated from L e L 2 10log L 10 8.7 where is the attenuation constant in Nepers per meter (Np/m). 15

Example: Cable Loss 50-W source is attached to a 50-W signal measurer with 300 ft of RG58U coaxial cable. The source is tuned to a frequency of 100 MHz, and the dial indicates an put of 15 m. t this frequency, the cable loss is 4.5 / 100 ft. Determine the (RMS) voltage at the input to the signal measurer in m. 16 10log 1 mw mw 10 v 20log 1μ μ 10

Example: Signal Source Output 50-W source is attached to a measurer whose input impedance is 25 W. The dial on the signal generator indicates that it is putting a level of 20 m. Determine the (RMS) voltage at the input to the signal measurer in m. 18