University of Utah Advanced Electromagnetics Green’s Function

Slides:



Advertisements
Similar presentations
Dr. Charles Patterson 2.48 Lloyd Building
Advertisements

2. Review of Matrix Algebra Dr. Ahmet Zafer Şenalp Mechanical Engineering Department Gebze Technical.
ELEN 3371 Electromagnetics Fall Appendix A: Tensors Instructor: Dr. Gleb V. Tcheslavski Contact: Office Hours:
Fundamentals of Applied Electromagnetics
Electromagnetism 2004 Fall Reference: 《 Electromagnetism, principles and application 》 by P.Lorrain & D.Corson.
1 Numerical ElectroMagnetics & Semiconductor Industrial Applications Ke-Ying Su Ph.D. National Central University Department of Mathematics 02. Method.
University of Utah Advanced Electromagnetics Green’s Function Dr. Sai Ananthanarayanan University of Utah Department of Electrical and Computer Engineering.
ECE M Introduction to Antennas and Antenna Systems
S. Mandayam/ EEMAG-1/ECE Dept./Rowan University Engineering Electromagnetics Fall 2004 Shreekanth Mandayam ECE Department Rowan University.
University of Utah Advanced Electromagnetics Image Theory Dr. Sai Ananthanarayanan University of Utah Department of Electrical and Computer Engineering.
University of Utah Advanced Electromagnetics Green’s Function Dr. Sai Ananthanarayanan University of Utah Department of Electrical and Computer Engineering.
reinisch_ Lecture #2 Electromagnetic Theory (Cravens, Appendix A)
S. Mandayam/ EEMAG-1/ECE Dept./Rowan University Engineering Electromagnetics Fall 2004 Shreekanth Mandayam ECE Department Rowan University.
Powerful tool For Effective study and to Understand Flow Devices…… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Tensor Notation.
Poynting’s Theorem … energy conservation John Henry Poynting ( )
Introduction to Physical Systems Dr. E.J. Zita, The Evergreen State College, 30.Sept.02 Lab II Rm 2272, Program syllabus,
Electromagnetic Waves Electromagnetic waves are identical to mechanical waves with the exception that they do not require a medium for transmission.
02/18/2015PHY 712 Spring Lecture 151 PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 15: Finish reading Chapter 6 1.Some details.
Methods of Math. Physics Dr. E.J. Zita, The Evergreen State College, 6 Jan.2011 Lab II Rm 2272, Winter wk 1 Thursday: Electromagnetism.
An introduction to Cartesian Vector and Tensors Dr Karl Travis Immobilisation Science Laboratory, Department of Engineering Materials, University of Sheffield,
EE 543 Theory and Principles of Remote Sensing
Chapter 1 - Vector Analysis. Scalars and Vectors Scalar Fields (temperature) Vector Fields (gravitational, magnetic) Vector Algebra.
Maxwell’s Equations If we combine all the laws we know about electromagnetism, then we obtain Maxwell’s equations. These four equations plus a force law.
Solution of Differential Equations
Hanjo Lim School of Electrical & Computer Engineering Lecture 2. Basic Theory of PhCs : EM waves in mixed dielectric.
Advanced Higher Mathematics Methods in Algebra and Calculus Geometry, Proof and Systems of Equations Applications of Algebra and Calculus AH.
Methods of Math. Physics Dr. E.J. Zita, The Evergreen State College Lab II Rm 2272, Winter wk 3, Thursday 20 Jan Electrostatics.
Chemistry 301/ Mathematics 251 Chapter 4
Advanced ElectromagneticsLN07_Green Functions 1 /35 Green's Functions.
Announcements Generalized Ampere’s Law Tested I I Consider a parallel plate capacitor that is being charged Try Ampere’s modified Law on two nearly identical.
1 Chapter 1 Introduction to Differential Equations 1.1 Introduction The mathematical formulation problems in engineering and science usually leads to equations.
Vectors scalar quantities magnitude mass temperature electric potential.
Maxwell’s Equations are Lorentz Invariant
EEE 431 Computational Methods in Electrodynamics Lecture 2 By Rasime Uyguroglu.
5. Electromagnetic Optics. 5.1 ELECTROMAGNETIC THEORY OF LIGHT for the 6 components Maxwell Eq. onde Maxwell.
Hanyang University 1/29 Antennas & RF Devices Lab. Partially filled wave guide Jeong Gu Ho.
CSE 681 Brief Review: Vectors. CSE 681 Vectors Direction in space Normalizing a vector => unit vector Dot product Cross product Parametric form of a line.
University of Utah Introduction to Electromagnetics Lecture 14: Vectors and Coordinate Systems Dr. Cynthia Furse University of Utah Department of Electrical.
Kankeshwaridevi Institute of Tech. Name of Students:rajput rahulsinh Enrollment no : Subject Code : Name Of Subject : Engineering Electromagnetics.
UPB / ETTI O.DROSU Electrical Engineering 2
ECE 305 Electromagnetic Theory
Warm up 1.) (3, 2, -4), (-1, 0, -7) Find the vector in standard position and find the magnitude of the vector.
ELEC 401 MICROWAVE ELECTRONICS Lecture 2
Advanced Higher Mathematics
Continuum Mechanics (MTH487)
ELEC 401 MICROWAVE ELECTRONICS Lecture 3
ELEC 401 MICROWAVE ELECTRONICS Lecture 3
Electromagnetic Radiation
Continuum Mechanics (MTH487)
Continuum Mechanics (MTH487)
Slide Presentations for ECE 329, Introduction to Electromagnetic Fields, to supplement “Elements of Engineering Electromagnetics, Sixth Edition” by Nannapaneni.
EEE 161 Applied Electromagnetics
Electromagnetic field tensor
Mehran University of Engineering & Technology SZAB khairpur campus
ELEC 401 MICROWAVE ELECTRONICS Lecture 3
ECE 305 Electromagnetic Theory
Finite Elements in Electromagnetics 4. Wave problems
Physics 111 Practice Problem Solutions 01 Units, Measurement, Vectors SJ 8th Ed.: Ch , 3.1 – 3.4 Contents: 1-7, 1-9, 1-10, 1-12, 1-15, 1-21* 3-5,
EEE 161 Applied Electromagnetics
ELEC 401 MICROWAVE ELECTRONICS Lecture 2
ME321 Kinematics and Dynamics of Machines
Related OSE's.
Numerical Computation and Optimization
Enumerations, Clamping, Vectors
Answer Grid – 3 & 4 Step Equations
Maxwell’s Equations and Plane Wave
Applied Electromagnetic Waves Notes 5 Poynting’s Theorem
Finish reading Chapter 6
1st Week Seminar Sunryul Kim Antennas & RF Devices Lab.
Finish reading Chapter 6
Presentation transcript:

University of Utah Advanced Electromagnetics Green’s Function Dr. Sai Ananthanarayanan University of Utah Department of Electrical and Computer Engineering www.ece.utah.edu/~psai

Time Harmonic Fields

Considering Homogeneous form:

Whereever singularities are present the frequencies of the excitation sorce matches the natural frequency of the system. This is referred to as resonance.

Green’s Identities and Methods Generalized procedure for obtaining Green’s Function for the three Dimentional partial differential equation

Green’s Identities and Methods

Green’s Function of Scalar Helmotz Equation

Substituting into:

Dyadic Green’s Function A dyad is a “rank two tensor”. In EM theory dyad is defined by the juxtaposition AB for vectors A and B With no dot or cross product between them.

Dyadic Green’s Function