전자장 일정표 9월 일 월 화 수 목 금 토 1 2 Lect. 1 3 4 5 6 7 Lect. 2, 3 8 9 Lect. 4

Slides:

Advertisements

Similar presentations

Polarization of EM waves

Advertisements

Lecture 23: Polarization

Now that we have determined the solutions to the differential equation describing the oscillations of the electric and magnetic fields with respect to.

Polarization - linear - circular

Microwave Devices E511 Lecture 2 Amr Al.Awamry. Agenda Plan waves in Lossless Medium Plan waves in general lossy Medium In Good conductor General Plan.

c = km/sec I F = I 0 x (cosθ) 2.

Physics 110G Waves TOC 1 Transverse Waves in Space Transverse Waves in Time Longitudinal Waves in Space Longitudinal Waves in Time.

Lecture No.11 By. Sajid Hussain Qazi. Andre Ampere.

The speed of light is a constant because the electric and magnetic fields support each other. If the speed of light was not constant energy would not be.

Prof. David R. Jackson Notes 17 Polarization of Plane Waves Polarization of Plane Waves ECE Spring 2013.

1 ECE 480 Wireless Systems Lecture 3 Propagation and Modulation of RF Waves.

Wireless Technology Lab., Kyung Hee University S-band Patch Antenna Design for CINEMA Chungju Kim

RS ENE 428 Microwave Engineering Lecture 3 Polarization, Reflection and Transmission at normal incidence 1.

Fundamental of Optical Engineering Lecture 7.  Boundary conditions:E and T must be continuous.  Region 1:

1 ECE 6345 Spring 2011 Prof. David R. Jackson ECE Dept. Notes 2.

Fundamentals of Electromagnetics: A Two-Week, 8-Day, Intensive Course for Training Faculty in Electrical-, Electronics-, Communication-, and Computer-

RS ENE 428 Microwave Engineering Lecture 3 Polarization, Reflection and Transmission at normal incidence 1.

Doc.: IEEE /0431r0 Submission April 2009 Alexander Maltsev, Intel CorporationSlide 1 Polarization Model for 60 GHz Date: Authors:

Review of Basic Polarization Optics for LCDs Module 4.

So far, we have considered plane waves in an infinite homogeneous medium. A natural question would arise: what happens if a plane wave hits some object?

ENE 429 Antenna and Transmission lines Theory

Solving Inequalities and their Graphs

Infokom. 3. ea szept Infocommunication systems Infokommunikációs rendszerek Lecture 3. előadás Radio transmission Rádiós átvitel Takács György.

Nonlinear Optics Lab. Hanyang Univ. Chapter 6. Processes Resulting from the Intensity-Dependent Refractive Index - Optical phase conjugation - Self-focusing.

Section 7.5 Trigonometric Equations Objective: To solve linear and quadratic trigonometric equations.

Sources (EM waves) 1.

Topics Use birefringence to generate and quantify elliptically polarized light. Understand, measure and characterize the optical activity of syrup.

1.4 Solving Inequalities I can: 1.Graph inequalities 2.Solve inequalities.

Magnetic Fields Due to Currents JH

Yonsei Univ. High-Speed Information Transmission Lab. Lect. 1-9-(1) Diffraction Grating (Mon.) ● Diffraction Grating d a a d ● ● ●● ● ●● ● ●●

Yonsei Univ. High-Speed Information Transmission Lab. Lect. 2-4 Optical Fiber (Mon.) d n2n2 n1n1 n2n2 Even solutions: Odd solutions: y=0 y=d/2.

Notes 16 ECE 6340 Intermediate EM Waves Fall 2015

Circle-Radius form By definition, a circle is the set of all points in a plane that lie a given distance from a given point. The given distance.

Click on this icon to start animation At the end of animation, ‘right click’ and select ‘end show’. Animation frame 1 of 32 To hasten the speed of animation,

ELEC 401 MICROWAVE ELECTRONICS Lecture 3

ELEC 401 MICROWAVE ELECTRONICS Lecture 3

Chapter 3 Polarization of Light Waves

NAME:-RAVIKANT KUMAR CLASS:-10 ROLL:-20.

Chapter 7 Section 1.

Is there B at the center? No, but there is curl of B. Demos: ru

Chapter 5. Polarization 第五章極化亞洲大學資訊工程學系碩士班呂克明教授二○○六年十月十六日

Edward C. Jordan Memorial Offering of the First Course under the Indo-US Inter-University Collaborative Initiative in Higher Education and Research: Electromagnetics.

Two Kinds of Polarized Light

Waves in Two Dimensions

ADINA INSTITUTE OF SCIENCE AND TECHNOLOGY

Chapter 13 Circles and Area

CH5: Radiative Properties of Natural Surfaces

6.1 to 6.3 Solving Linear Inequalities

Link Analysis C/N Uplink (Uplink Carrier to Noise Ratio) C/N Downlink

Brief introduction to Partial Differential Equations (PDEs)

Ordinary light versus polarized light

To use it you will have to provide the narration.

“If you give a mouse a cookie” Format

ELECTROMAGNETIC WAVE PROPAGATION Polarization

Matrix treatment of polarization

Unit 1 Representing Real Numbers

Propagating Monochromatic Gaussian Beam Wave with

INEQUALITIES Many Kinds of Inequalities : Linear Inequalities

Warm-up: HW: Cumulative Review Packet

Lecture 6: Surface Integrals

ENE 428 Microwave Engineering

1.3:Solving and Graphing Linear Inequalities

Slide Presentations for ECE 329, Introduction to Electromagnetic Fields, to supplement “Elements of Engineering Electromagnetics, Sixth Edition” by Nannapaneni.

Channel Modeling with PAA Orientations

plane waves in lossy material

Presentation transcript:

전자장 일정표 9월 일 월 화 수 목 금 토 1 2 Lect. 1 3 4 5 6 7 Lect. 2, 3 8 9 Lect. 4 10 11 Lect. 5, 6 (11-1, B039) 12 13 Tutorial 6-7, B039 14 Lect. 7, 8 15 16 Lect. 9 17 18 19 20 Tutorial 6-7, B039 21 Lect. 10,11 22 23 Q/A Test#1 7-9 at C040 24 25 26 27 추 28 석 29 30 Test #1 Solutions

Yonsei Univ. High-speed information transmission Lab. Lect. 4 Polarization Time varying characteristics of E-field direction Consider How does E-field direct change in time at Z=0? (What is its polarization?) 1) E1=0 and E2= not(0) 이면  y ※ E-field 는 y축 방향으로 왕복운동 Linear polarization (Animation) x What if E1 = E2? Yonsei Univ. High-speed information transmission Lab.

Yonsei Univ. High-speed information transmission Lab. Lect. 4 Polarization 2) E2 = j E1 and E1 real y ※ E-field traces a circle: See Animation x Circular polarization (RHCP) What if E2 = -jE1 and E1 real ? LHCP Take the propagation direction (-z in this case) as reference: Right Hand Circular Polarization (RHCP) or Left Hand Circular Polarization (LHCP) Yonsei Univ. High-speed information transmission Lab.

Yonsei Univ. High-speed information transmission Lab. Lect. 4 Polarization 3) In general, y In elliptical polarization, both magnitude and direction change. Can be right-handed or left-handed Depending on sign of x ※ HW) Prob. 1-b in 1999 test 1 Yonsei Univ. High-speed information transmission Lab.