ELEC 351 Notes Set #18

Similar documents
Path (space curve) Osculating plane

Study Material with Classroom Practice solutions. To Electromagnetic Theory CONTENTS. 01 Static Fields Maxwell Equations & EM Waves 06 11

Lecture 35. Diffraction and Aperture Antennas

ELEG 413 Lecture #6. Mark Mirotznik, Ph.D. Professor The University of Delaware

School of Electrical Engineering. Lecture 2: Wire Antennas

Part II, Measures Other Than Conversion I. Apr/ Spring 1

C-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0)

Physics 202, Lecture 5. Today s Topics. Announcements: Homework #3 on WebAssign by tonight Due (with Homework #2) on 9/24, 10 PM

Fluids & Bernoulli s Equation. Group Problems 9

E. Computation of Permanent Magnetic Fields

(A) 6.32 (B) 9.49 (C) (D) (E) 18.97

Electric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin

Theory of Spatial Problems

SPHERICAL COORDINATE SYSTEMS FOR DEFINING DIRECTIONS AND POLARIZATION COMPONENTS IN ANTENNA MEASUREMENTS

Chapter 4 Circular and Curvilinear Motions

Mark Scheme (Results) January 2008

MASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS

Lecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture:

Chapter 2 Reciprocal Lattice. An important concept for analyzing periodic structures

Class Summary. be functions and f( D) , we define the composition of f with g, denoted g f by

Mon. Tues. 6.2 Field of a Magnetized Object 6.3, 6.4 Auxiliary Field & Linear Media HW9

In Review: A Single Cycle Datapath We have everything! Now we just need to know how to BUILD CONTROL

EECE 260 Electrical Circuits Prof. Mark Fowler

Aakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics

Chapter 7 Electrodynamics

Planar Upward Drawings

Electricity & Magnetism Lecture 6: Electric Potential

( ) ( ) ( ) ( ) ( ) # B x ( ˆ i ) ( ) # B y ( ˆ j ) ( ) # B y ("ˆ ( ) ( ) ( (( ) # ("ˆ ( ) ( ) ( ) # B ˆ z ( k )

sin sin 1 d r d Ae r 2

1. Viscosities: μ = ρν. 2. Newton s viscosity law: 3. Infinitesimal surface force df. 4. Moment about the point o, dm

Ch 1.2: Solutions of Some Differential Equations

E F. and H v. or A r and F r are dual of each other.

EECE 301 Signals & Systems Prof. Mark Fowler

Physics 604 Problem Set 1 Due Sept 16, 2010

Physics 1502: Lecture 2 Today s Agenda

Multi-Section Coupled Line Couplers

3.1 General solutions for TEM, TE and TM waves Procedure to analyze a TEM (Ez, Hz=0) line

Course Updates. Reminders: 1) Assignment #8 available. 2) Chapter 28 this week.

Waveguide Guide: A and V. Ross L. Spencer

Physics 11b Lecture #11

Bf: the positive charges in the moving bar will flow downward

Midterm Exam. CS/ECE 181B Intro to Computer Vision. February 13, :30-4:45pm

Physics 9 Fall 2011 Homework 2 - Solutions Friday September 2, 2011

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 8: Effect of a Vertical Field on Tokamak Equilibrium

(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information

TOPIC 5: INTEGRATION

CSE303 - Introduction to the Theory of Computing Sample Solutions for Exercises on Finite Automata

Dynamically Equivalent Systems. Dynamically Equivalent Systems. Dynamically Equivalent Systems. ME 201 Mechanics of Machines

This immediately suggests an inverse-square law for a "piece" of current along the line.

set is not closed under matrix [ multiplication, ] and does not form a group.

10 m, so the distance from the Sun to the Moon during a solar eclipse is. The mass of the Sun, Earth, and Moon are = =

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface

PH672 WINTER Problem Set #1. Hint: The tight-binding band function for an fcc crystal is [ ] (a) The tight-binding Hamiltonian (8.

Homework Assignment 3 Solution Set

Accretion disks around rotating black holes. (c)2017 van Putten 1

Section 35 SHM and Circular Motion

Radial geodesics in Schwarzschild spacetime

π,π is the angle FROM a! TO b

Simple Harmonic Motion I Sem

CHAPTER TWO MULTIPLE INTEGRAL

RF circuits design Grzegorz Beziuk. Introduction. Basic definitions and parameters. References

UNIT-4. File downloaded from For the things of this world cannot be made known without a knowledge of mathematics.

Jens Als-Nielsen, Copenhagen University. X-ray Physics. Cheiron School 2009

Chapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s:

Elliptical motion, gravity, etc

GRAVITATION 4) R. max. 2 ..(1) ...(2)

GUC (Dr. Hany Hammad)

(, ) which is a positively sloping curve showing (Y,r) for which the money market is in equilibrium. The P = (1.4)

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

U>, and is negative. Electric Potential Energy

Who is this Great Team? Nickname. Strangest Gift/Friend. Hometown. Best Teacher. Hobby. Travel Destination. 8 G People, Places & Possibilities

Week 8. Topic 2 Properties of Logarithms

SOLUTIONS FOR ADMISSIONS TEST IN MATHEMATICS, COMPUTER SCIENCE AND JOINT SCHOOLS WEDNESDAY 5 NOVEMBER 2014

On the diagram below the displacement is represented by the directed line segment OA.

Math 10 - Unit 5 Final Review - Polynomials

SUMMER KNOWHOW STUDY AND LEARNING CENTRE

SSC Mains Mock Test 226 [Answer with Solution]

Optimization. x = 22 corresponds to local maximum by second derivative test

Vector Calculus Identities

Picking Coordinate Axes

temperature T speed v time t density ρ scalars may be constant or may be variable yes distributive a(b+c) = ab+ac

Lecture 4. Conic section

Dielectric Waveguide 1

REVIEW Chapter 1 The Real Number System

Walk Like a Mathematician Learning Task:

Classwork. Example 1 S.35

Chapter 21: Electric Charge and Electric Field

Collisionless Hall-MHD Modeling Near a Magnetic Null. D. J. Strozzi J. J. Ramos MIT Plasma Science and Fusion Center

If C = 60 and = P, find the value of P. c 2 = a 2 + b 2 2abcos 60 = a 2 + b 2 ab a 2 + b 2 = c 2 + ab. c a

CHAPTER 5 CIRCULAR MOTION

SSC [PRE+MAINS] Mock Test 131 [Answer with Solution]

Let s celebrate! UNIT. 1 Write the town places. 3 Read and match. school. c 1 When s your birthday? Listen, check and practise the dialogues.

". :'=: "t',.4 :; :::-':7'- --,r. "c:"" --; : I :. \ 1 :;,'I ~,:-._._'.:.:1... ~~ \..,i ... ~.. ~--~ ( L ;...3L-. ' f.':... I. -.1;':'.

PH427/PH527: Periodic systems Spring Overview of the PH427 website (syllabus, assignments etc.) 2. Coupled oscillations.

Answers to test yourself questions

Lecture 11: Potential Gradient and Capacitor Review:

ANTENNAS. Vector and Scalar Potentials. Maxwell's Equations. D = εe. For a linear, homogeneous, isotropic medium µ and ε are contant.

ME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören

ragsdale (zdr82) HW2 ditmire (58335) 1

EE243 Advanced Electromagnetic Theory Lec # 22 Scattering and Diffraction. Reading: Jackson Chapter 10.1, 10.3, lite on both 10.2 and 10.

Transcription:

Assignmnt #8 Poblm 9. Poblm 9.7 Poblm 9. Poblm 9.3 Poblm 9.4 LC 35 Nots St #8 Antnns gin nd fficincy Antnns dipol ntnn Hlf wv dipol Fiis tnsmission qution Fiis tnsmission qution Do this ssignmnt by Novmb 9. Mk-up Tutoil Tusdy Dcmb 4 8 Th mk-up tutoil will b t th sm tim nd in th sm oom s th usul Mondy tutoil. Not tht th will b tutoils on both Mondy Dcmb 3 nd on Tusdy Dcmb 4. Th finl xm in LC 35 is Dcmb 3 8 fom : to 5:.

Th F Filds of n Antnn ( ) ( ) + ( )

Find th Mgntic Fild In th f fild th lctic fild is: ( ) ( ) + ( ) Wht is th mgntic fild in th f fild? Fdy s Lw: so x ωµ H H ωµ Do th cul in sphicl coodints. Nglct th tms in / nd / 3 bcus thy n fild.

Cul in sphicl coodints: lctic fild: ( ) ( ) ( ) + ( ) sin sin ( ) + sin ( ) +

Th componnts of th f fild : ( ) sin sin sin sin ( ) ( ) ( ) ( ) sin sin ( ) ( ) sin sin Th componnt vis s so w cn nglct it. â Wok on th componnt: â

Th componnts of th f fild : ( ) ( ) Wok on th componnt: â ( ) () sin sin ( ) ( ) ( )

Th componnts of th f fild : ( ) ( ) Wok on th componnt: â ( ) () ( ) ( )

So th cul is vlutd s: + And th mgntic fild is: H ωµ + H ωµ H ωµ µ ε µ µε µ µε ωµ µε ω ωµ ωµ

So th mgntic fild is: H + ( ) ( ) + ( ) ( ) H + Hnc in th f fild of ny ntnn:

Pow Flow Dnsity ( ) ( ) ( ) + ( ) ( ) ( ) H + [ ] * R H S v + + * R S v + + S v * * R conugt conugt

+ + S v * * R S v * * R + S v * * R + R S v + S v Wtts p squ mt

3 Qusi-Pln Wvs ( ) ( ) ( ) + ( ) ( ) ( ) H + ( ) ( ) ( ) ( ) H S v S v ( ) ( ) ( ) ( ) H nd HH nd HH

Th Htzin Dipol Pul Whits nd Ns Fig. 9.3 4

Th Htzin Dipol << λ 5

N Filds nd F Filds 6

Th N Fild 7

Th F Fild 8

Angl Dpndnc I sin 4π ( ) ( ) + ( ) I 4π ( ) sin nd

Th Dipol Antnn

Th F Filds of Dipol Antnn It My B Shown tht: ( ) ( ) I π ( ) F( ) I π ( ) F( )

Hlf-Wv Dipol Antnn In gnl: I π ( ) F( ) Hlf-wv dipol: F F h ( ) ( ) π λ λ cos h π λ π h λ 4 λ 4 ( hcos ) cos( h) sin π π cos cos cos sin

F ( ) π π cos cos cos sin F ( ) π cos cos sin I π ( ) F( )

xmpl

Ointtion- vticl dipol nd hoizontl pln I π ( ) F( ) Th dipol is t th oigin ointd long th z xis which is th vticl xis. Th hoizontl pln is th xy pln 9.

Hlf-Wv Dipol Antnn Fom bov: I π ( ) F( ) F ( ) π cos cos sin

F π cos cos sin π π cos cos π sin cos ( )

wh F ( ) π cos cos sin

6 ππ 3 d F ( ) π F 3 π cos cos sin π π cos cos 3 π sin 3.865

Rviw: F Fild of n Antnn ( ) ( ) + ( ) ( ) H + + S v Th pow flow dnsity: Wtts/mt

Rviw: Th F Filds of Dipol Antnn It My B Shown tht: ( ) ( ) I π ( ) F( )

Rdition Pttns ( ) ( ) + ( ) Azimuth Pttn fo: 9 : nd vs. (xy pln) lvtion pttn fo : nd vs. (xz pln) lvtion pttn fo 9 : nd vs. (yz pln)

I π ( ) F( ) F ( ) π cos cos sin

π π π π I F I cos sin cos cos π π π π F so ( ) π sin cos cos F

I π ( ) F( ) I π π cos cos sin

Amplitud vs. Position 48

Ay of Two Dipols Fo ch individul dipol: ππ II ooff FF cos ππ cos sin In th zimuth o 9 dgs pln FF cos ππ cos ππ sin ππ cos Hnc w cn wit mo simply s CCII oo wh CC ππ And th distnc fom th dipol to th obsv.

Ay of Two Dipols continud II oo δδ # # II oo Fo dipol # t th oigin th cunt is II oo nd th fild stngth is CCII oo RR RR RR th distnc fom dipol # to th obsv. An ntnn y is md up of two vticl hlf-wv dipol ntnns. Antnn # is t th oigin nd cis cunt II oo. Antnn # is t xx dd nd cis cunt II oo δδ with phs shift of δδ ltiv to ntnn #. Find th f fild. Fo dipol # t xx dd th cunt is II oo δδ nd th fild stngth is: CCII oo δδ RR RR RR th distnc fom dipol # to th obsv. Fo two dipols cting togth us supposition: CCII oo RR RR RR δδ + CCII oo RR Cn w simplify this fo n obsv in th f fild?

Ay of Two Dipols: F Fild Appoximtion # # CI R R R R d cos + CI δ R wh is th distnc fom th oigin to th obsv. Fo ntnn # RR is smll thn : R Fo mplitud nglct dd cos compd to. But fo phs puposs w cnnot nglct dd cos bcus it my b significntly-lg phs ngl such s 9 dgs o 8 dgs. CI CI + CI + CI + δ δ ( d cos ) d cos ( d cos ) ( ) ( δ d cos CI )

nd Fi Ay: dition in th +x diction. + ( ) ( δ d cos CI ) Choos π δ λ d 4 π λ π d λ 4 CCII oo Ninty dgs out of phs. Spc th ntnns qut-wvlngth pt. + ππ ππ cos

In th Obsv t Zo Dgs + x diction fo cos + cos ( ) CI π π CI + + π π π π cos ( ) CI CI CI ( + ) CI CCII oo ππ ππ cos II oo CCII oo

In th Obsv t 8 Dgs + + π π π π cos8 ( ) π CI CI CI ( + ) x diction fo 8 8 cos8 cos ( ) CI + π π CI CCII oo ππ ππ cos ππ II oo CCII oo

Amplitud vs. Position

Cdioid Rdition Pttn

Bodsid Ay: dition in th +y nd y diction. + ( ) ( δ d cos CI ) Choos: δ λ d π λ d π λ + Opt th ntnns in phs Spc th ntnns hlf-wvlngth pt ( ) ( π cos CI ) δ

Obsv t 9 Dgs CI π cos9 ( 9) CI ( + ) CI ( + ) CI ( + ) + ( ) ( π cos CI ) 9 cos 9 Th filds in phs nd dd nd so th is mximum fild stngth fo 9 dgs.

Obsv t Zo Dgs + ( ) ( π cos CI ) cos ( ) ( π cos ) ( π CI + CI + ) CI ( ) Th filds out of phs nd subtct nd so th is zo fild fo dgs.

Amplitud vs. Position

Rdition Pttn

Dictionl Accss-Point Antnn

Th is blun on th oth sid: Blun blnc to unblnc tnsfom. Th ntnn is blncd Th coxil cbl is unblncd. 79

Rdition Pttn of th Dictionl AP Antnn