Electromagnetic (EM) Wave

Slides:



Advertisements
Similar presentations
Maxwell’s Equations & EMR.
Advertisements

EMLAB 1 Introduction to electromagnetics. EMLAB 2 Electromagnetic phenomena The globe lights up due to the work done by electric current (moving charges).
My Chapter 22 Lecture.
Electromagnetic Waves
Alternating Current Circuits And Electromagnetic Waves Chapter 21.
Chapter 29 Continued-Chapter 31- Chapter EMF Induced in a Moving Conductor Example 29-8: Force on the rod. To make the rod move to the right.
Physics 1402: Lecture 26 Today’s Agenda Announcements: Midterm 2: NOT Nov. 6 –About Monday Nov. 16 … Homework 07: due Friday this weekHomework 07: due.
Let’s review electromagnetism. Electric Generator.
Waves can be represented by simple harmonic motion.
Antennas. Free Charge  A free charge has a constant electric field and no magnetic field.  No waves are produced. No radiationNo radiation  A charge.
Physics II PHY 202/222 Magnetism
Radio 1 Radio. Radio 2 Observations about Radio Transmit sound long distances without wires Transmit sound long distances without wires Involve antennas.
Electricity, Electronics And Ham Radio “Kopertroniks” By Nick Guydosh 4/12/07.
Lecture 2: Radio Wave Propagation
& Electromagnetic Waves.  equivalent to Coulomb’s law.
1 Faraday’s Law Chapter Ampere’s law Magnetic field is produced by time variation of electric field.
Antennas and Propagation Lecture 15. Overview Electric and Magnetic Field Coupling EM Radiations Period, Frequency, and Wavelength Phase Lag and Phase.
Electromagnetic Waves Chapter Introduction: Maxwell’s equations Electricity and magnetism were originally thought to be unrelated Electricity.
Chapter 9 Electromagnetic Waves. 9.2 ELECTROMAGNETIC WAVES.
Why does my circuit radiate? Presented by Paul Edwards.
Electromagnetic Waves Chapter 35. Electromagnetic (EM) Waves Can travel through space Radio, Microwaves, IR, Light, UV, X-rays, Gamma Rays All on the.
1 Chapter 3 Electromagnetic Theory, Photons and Light September 5,8 Electromagnetic waves 3.1 Basic laws of electromagnetic theory Lights are electromagnetic.
Chapter 21 Electromagnetic Waves. General Physics Exam II Curve: +30.
Chapter 4 Electromagnetic Waves. 1. Introduction: Maxwell’s equations  Electricity and magnetism were originally thought to be unrelated  in 1865, James.
PHYS 1442 – Section 004 Lecture #16 Weednesday March 19, 2014 Dr. Andrew Brandt Chapter 22 Maxwell and the c.
Physics 1202: Lecture 18 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, etc.
Maxwell’s Equations and Electromagnetic Waves
Concept of Radiation Chapter 3. Chapter Outlines Chapter 3 Concept of Radiation  Radiation Mechanism  Basic Radiation Source – Single Wire  Basic Radiation.
Wave Dispersion EM radiation Maxwell’s Equations 1.
Chapter Concept of Radiation.
Physics 213 General Physics Lecture 14. Test 1 1. Click in!!
Chapter 5 Electromagnetic Waves. 1. Introduction: Maxwell’s equations  Electricity and magnetism were originally thought to be unrelated  in 1865, James.
1Electromagnetic Waves.  Administrative ◦ Quiz Today ◦ Review Exam Grades ◦ Review Exam  Begin Chapter 23 – Electromagnetic Waves  No 10:30 Office.
SACE Stage 2 Physics Light and Matter Electromagnetic Waves.
ELECTROMAGNETIC WAVES. Current can be induced in a coil by a changing magnetic field. A changing magnetic field induces a changing electric field at right.
Physics 213 General Physics Lecture Last Meeting: Electric Generators, Alternating Current Today: Electromagnetic Waves, Maxwell’s Equations.
Antennas/Antenna Arrays
Reading Quiz #17 1) EMF stands for … Electromagnetic force
Introduction to electromagnetics
Two questions: (1) How to find the force, F on the electric charge, Q excreted by the field E and/or B? (2) How fields E and/or B can be created?
Lecture 19 Electromagnetic Waves.
Electromagnetic Waves
ECEN5341/4341 Spring 2017 Lecture 2 January 20,2017.
Electromagnetic Waves
Electromagnetic Radiation
Electromagnetic Radiation
Electromagnetism 1865: James Clerk Maxwell 1887: Heinrich Hertz
From last time… Faraday: Inductance: flux = (inductance) x (current)
PLANE WAVE PROPAGATION
Lecture 14 : Electromagnetic Waves
The equations so far..... Gauss’ Law for E Fields
Maxwell’s Equations and Electromagnetic Waves
Electromagnetic waves
Chapter 23: Electromagnetic Waves
General Physics (PHY 2140) Lecture 22 Electricity and Magnetism
Electromagnetic Waves
Phys102 Lecture 20 Electromagnetic Waves * (skipped)
Electricity, Magnetism 15 September 2015 presented by Prof. Geller
Chapter 3 Electromagnetic Theory, Photons and Light
Electromagnetism & EM Waves
ENE 325 Electromagnetic Fields and Waves
Lecture 12 Optical Properties Md Arafat Hossain Outlines.
Wireless Communications Chapter 4
Two questions: (1) How to find the force, F on the electric charge, Q excreted by the field E and/or B? (2) How fields E and/or B can be created?
Maxwell’s Equations and Electromagnetic Waves
Abasaheb Kakade Art’s & Science College Bodhegaon
ECEN5341/4341 Spring 2019 Lecture 2 January 16,2019.
Electromagnetism & EM Waves
Electromagnetism & EM Waves
1st Week Seminar Sunryul Kim Antennas & RF Devices Lab.
Presentation transcript:

How does an antenna that only generates a magnetic field, generate an electromagnetic (EM) wave?

Electromagnetic (EM) Wave Made up of two time varying components: Electric field (E) Magnetic field (B) Electric and magnetic fields Orthogonal and in phase Are tightly coupled to each other Propagate through space at the speed of light How do we know this: Maxwell’ equations Greatest physicists all time: Newton (F= ma) Einstein (E= mc2) ?

Electromagnetic (EM) Wave Made up of two time varying components: Electric field (E) Magnetic field (B) Electric and magnetic fields Orthogonal and in phase Are tightly coupled to each other Propagate through space at the speed of light How do we know this: Maxwell’ equations Greatest physicists all time: Newton (F= ma) Einstein (E= mc2) Maxwell (Maxwell’s equations)

Force Fields & EM Waves Charged particle: free electron (which has a negative charge) Constant electric field is produced by a stationary charged particle Example: a capacitor with a DC charge Constant magnetic field is produced by a moving charged Important point: charges are moving at a constant velocity Example: a DC current flowing thru a conductor An EM wave is produced by an accelerating charged particle Examples: Particle accelerator AC current flowing thru a conductor of sufficient length

Why Are Maxwell’s Equations Important Show the link between electricity, magnetism and light Show that light is a form of EM radiation Break down under some conditions Led Einstein to Theory of Relativity Mathematical description of how EM waves are generated and altered

How Does An EM Wave Get Generated From Maxwell’s equations: A time varying electric field induces a time varying magnetic field A time varying magnetic field induces a time varying electric field This interplay between induced electric and induced magnetic fields leads to propagating electromagnetic waves Most antennas do not launch an EM wave They generate either a time varying electric field or a time varying magnetic field

Spatial Fields (Distance From An Antenna) Pure EM waves only exist in the Far Field

Spatial Fields (Distance From An Antenna) Pure EM waves only exist in the Far Field MHz 3.5 175 ft 144 4.3 ft 564 ft 14 ft

EM Wave From A Magnetic Field Generator Conductor length must be > 0.05 wavelength to radiate (LC tank circuits don’t radiate because they are << 0.05 wavelength) Initially: E & B fields are orthogonal but 90o out of phase Energy goes back and forth between E & B fields No radiation Analogous to a lossless LC tank circuit Reactive Near-field

EM Wave From A Magnetic Field Generator Length must be > 0.05 wavelength to start radiating (This is why LC tank circuits don’t radiate) Reactive Near-field Radiating Near Field (Transition region)

EM Wave From A Magnetic Field Generator Length must be > 0.05 wavelength to start radiating (This is why LC tank circuits don’t radiate) E & B fields in-phase Full radiation No reactive energy Far Field

Magnetic Loop Antenna RF Far Field Pattern Reactive Near-field

Electric Field Antenna + DC E Field -

Electric Field Antenna L> 0.05 wavelength + L/2 + => => DC E Field RF E Field - L/2 - Reactive Near-field

Magnetic Loop Antenna Why is it called a Magnetic Loop antenna? In the reactive near-field: It generates a magnetic field on transmit and, It responds primarily to the magnetic field of an EM wave when receiving In the far field, there is no difference between the EM wave generated from a magnetic loop or from a dipole Ground effects: Near field: detuning and losses are minimal Far field: similar to ground mounted vertical Pseudo-Brewster angle notch-out