Review of basic EM concepts

Slides:



Advertisements
Similar presentations
Today’s summary Polarization Energy / Poynting’s vector
Advertisements

NASSP Self-study Review 0f Electrodynamics
ENE 428 Microwave Engineering
Chapter 1 Electromagnetic Fields
PH0101 UNIT 2 LECTURE 31 PH0101 Unit 2 Lecture 3  Maxwell’s equations in free space  Plane electromagnetic wave equation  Characteristic impedance 
Electromagnetic (E-M) theory of waves at a dielectric interface
So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures.
What is a wave? f(x) f(x-3) f(x-2) f(x-1) x
Chung-Ang University Field & Wave Electromagnetics CH 8. Plane Electromagnetic Waves 8-4 Group Velocity 8-5 Flow of Electromagnetic Power and the Poynting.
Feb. 2, 2011 Rosseland Mean Absorption Poynting Vector Plane EM Waves The Radiation Spectrum: Fourier Transforms.
08/28/2013PHY Lecture 011 Light is electromagnetic radiation! = Electric Field = Magnetic Field Assume linear, isotropic, homogeneous media.
Chapter 33. Electromagnetic Waves What is Physics? Maxwell's Rainbow The Traveling Electromagnetic Wave, Qualitatively The Traveling.
The Electromagnetic Field. Maxwell Equations Constitutive Equations.
Nonlinear Optics Lab. Hanyang Univ. Nonlinear Optics ( 비선형 광학 ) 담당 교수 : 오 차 환 교 재 : A. Yariv, Optical Electronics in Modern Communications, 5 th Ed., Oxford.
Wave Motion & EM Waves (IV)
Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Classical electrodynamics.
1 Chapter 3 Electromagnetic Theory, Photons and Light September 5,8 Electromagnetic waves 3.1 Basic laws of electromagnetic theory Lights are electromagnetic.
In the absence of sources, the Maxwell equations in an infinite medium are.
Lecture/Lab: Interaction of light with particles. Mie’s solution.
Linear optical properties of dielectrics
Classical Optics Prof. D. Rich
Introduction to materials physics #3
PHYS 408 Applied Optics (Lecture 3) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
Lecture 2. Review lecture 1 Wavelength: Phase velocity: Characteristic impedance: Kerchhoff’s law Wave equations or Telegraphic equations L, R, C, G ?
RS ENE 428 Microwave Engineering Lecture 2 Uniform plane waves.
PHYS 408 Applied Optics (Lecture 4) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
ELEN 340 Electromagnetics II Lecture 2: Introduction to Electromagnetic Fields; Maxwell’s Equations; Electromagnetic Fields in Materials; Phasor Concepts;
5. Electromagnetic Optics. 5.1 ELECTROMAGNETIC THEORY OF LIGHT for the 6 components Maxwell Eq. onde Maxwell.
EE231 Introduction to Optics: Basic EM Andrea Fratalocchi ( slide 1 EE 231 Introduction to Optics Review of basic EM concepts Andrea.
Lecture 6: Maxwell’s Equations
UPB / ETTI O.DROSU Electrical Engineering 2
Chapter 1 Electromagnetic Fields
Plane electromagnetic waves
ELEC 401 MICROWAVE ELECTRONICS Lecture 2
Electromagnetic Waves
PHYS 408 Applied Optics (Lecture 3)
ELEC 401 MICROWAVE ELECTRONICS Lecture 3
ENE 428 Microwave Engineering
Chapter 11. The uniform plane wave
Maxwell’s Equations.
Maxwell’s Equation.
ELEC 401 MICROWAVE ELECTRONICS Lecture 3
ELEC 401 MICROWAVE ELECTRONICS Lecture 3
Review of basic EM concepts
Light Waves and Polarization
PLANE WAVE PROPAGATION
Lecture 14 : Electromagnetic Waves
ELEC 401 MICROWAVE ELECTRONICS Lecture 3
The equations so far..... Gauss’ Law for E Fields
ECE 305 Electromagnetic Theory
Chapter 33. Electromagnetic Waves
Eng. Mohamed Ossama Ashour
ELEC 401 MICROWAVE ELECTRONICS Lecture 2
ENE 325 Electromagnetic Fields and Waves
Chapter 3 Electromagnetic Theory, Photons and Light
Geometrical optics and Imaging theory
Scalar theory of diffraction
Electromagnetic waves
Scalar theory of diffraction
Scalar theory of diffraction
Scalar theory of diffraction
Scalar theory of diffraction
PHYS 408 Applied Optics (Lecture 4)
Scalar theory of diffraction
Scalar theory of diffraction
Scalar theory of diffraction
Optics 430/530, week II Plane wave solution of Maxwell’s equations
1st Week Seminar Sunryul Kim Antennas & RF Devices Lab.
Presentation transcript:

Review of basic EM concepts EE 231 Introduction to Optics Review of basic EM concepts Lesson 1 Andrea Fratalocchi www.primalight.org

Light matter interactions in isotropic and homogeneous media EM Field Maxwell Equations Material response EM sources Constitutive relations

Light matter interactions in isotropic and homogeneous media Magnetic constant Constitutive relations Refractive index Permittivity Susceptibility Dielectric constant Material polarization Material response Input field

Light matter interactions in isotropic and homogeneous media Work done by EM field x unit volume and x unit time By using the vector identity Poynting Theorem

Light matter interactions in isotropic and homogeneous media Poynting Theorem Energy flux of EM field, or equivalently, power density x unit area is direction of Energy density of the EM field Energy conservation equation for EM field

Light matter interactions in isotropic and homogeneous media Question: why energy is a fundamental quantity?

Light matter interactions in isotropic and homogeneous media Question: why energy is a fundamental quantity? Because is related to the concept of norm, which is related to the fundamental concept of "length": This is a general result: Power dissipated in circuits: Depends on the norm of the signal Energy of elastic system (e.g., spring):

Light matter interactions in isotropic and homogeneous media Question: did you already encounter expressions of this type?

Light matter interactions in isotropic and homogeneous media Question: did you already encounter expressions of this type? Schroedinger equation of a free electron Conservation of number of particles

Light matter interactions in isotropic and homogeneous media Complex formalism Time average of complex functions

Light matter interactions in isotropic and homogeneous media Optical Intensity Average power x unit area carried by the EM field in the direction of propagation of the energy The intensity is one of the most important optical quantity In the complex formalism: Exercise: demonstrate this relation Question: why we use the intensity and not directly the EM field?

Light matter interactions in isotropic and homogeneous media Plane waves A harmonic plane wave is a constant-frequency wave whose wavefronts (surfaces of constant phase) are infinite parallel planes of constant peak-to-peak amplitude normal to the phase velocity vector. Wave description of a plane wave Maxwell equations

Light matter interactions in isotropic and homogeneous media Maxwell equations Wave description of a plane wave Frequency Wavevector For a plane wave, we have Dispersion relation By substituting into Maxwell equations Key quantity, this specific expression is valid only in isotropic and homogenous materials

Light matter interactions in isotropic and homogeneous media Maxwell equations Wave description of a plane wave Linearly polarized plane wave From Maxwell equations Vacuum impedance

Light matter interactions in isotropic and homogeneous media Maxwell equations Wave description of a plane wave Exercise: demonstrate that the unit vectors of k, E, H are mutually orthogonal

Light matter interactions in isotropic and homogeneous media Maxwell equations Wave description of a plane wave Exercise: demonstrate that the unit vectors of k, E, H are mutually orthogonal Is orthogonal to k and E

Light matter interactions in isotropic and homogeneous media Maxwell equations Wave description of a plane wave Exercise calculate the direction and the norm of the Poynting vector

Light matter interactions in isotropic and homogeneous media Maxwell equations Wave description of a plane wave Exercise calculate the direction and the norm of the Poynting vector The direction of the energy is parallel to the wave vector. This is NOT a general property of plane waves, and is valid only in isotropic media

Light matter interactions in isotropic and homogeneous media Homework 1: You are studying the emission of a unknown type of optical source. From your analysis, the field emission from the source is characterized by the following time dependent waveform: With arbitrary N integer. How many different colors are contained in such optical field? (Hint: start by plotting and analyzing the field profile for different N)

Light matter interactions in isotropic and homogeneous media Homework 2: Demonstrate this relationship:

Light matter interactions in isotropic and homogeneous media Homework 3: Expand the following expression into simple exponentials:

Light matter interactions in isotropic and homogeneous media References A. Yariv, Optical electronics in modern communication, 6th Edition, Chapter 1 Any textbook of classical EM theory