P30 - 1 Workshop: Using Visualization in Teaching Introductory E&M AAPT National Summer Meeting, Edmonton, Alberta, Canada. Organizers: John Belcher, Peter.

Slides:



Advertisements
Similar presentations
Maxwell’s Equations The two Gauss’s laws are symmetrical, apart from the absence of the term for magnetic monopoles in Gauss’s law for magnetism Faraday’s.
Advertisements

Chapter 29: Maxwell’s Equations and Electromagnetic Waves
Short Version : 29. Maxwell’s Equations & EM Waves
Maxwell’s Equations and Electromagnetic Waves
Chapter 22 Electromagnetic Waves. Units of Chapter 22 Changing Electric Fields Produce Magnetic Fields; Maxwell’s Equations Production of Electromagnetic.
My Chapter 22 Lecture.
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? Gauss’s.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 22: Electromagnetic Waves Production.
Chapter 4: Wave equations
1 W15D1: Poynting Vector and Energy Flow Today’s Readings: Course Notes: Sections 13.6,
Electromagnetic Waves
Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com.
Chapter 22: Electromagnetic Waves
VI–2 Electromagnetic Waves Main Topics Properties of Electromagnetic Waves: Generation of electromagnetic waves Relations of.
P Workshop: Using Visualization in Teaching Introductory E&M AAPT National Summer Meeting, Edmonton, Alberta, Canada. Organizers: John Belcher, Peter.
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.
PHYSICS 231 INTRODUCTORY PHYSICS I
Physics for Scientists and Engineers II, Summer Semester Lecture 21: July 13 th 2009 Physics for Scientists and Engineers II.
P W15D2 Poynting Vector and EM Waves Radiation Pressure Final Exam Review.
adapted from (nz302.jpg)
P Technology Enabled Active Learning (TEAL) Learning without Barriers / Technology without Borders Symposium December 2, 2006 John Belcher, Peter.
1 W14D1: EM Waves, Dipole Radiation, Polarization and Interference Today’s Reading Course Notes: Sections 13.8, 13.10,
Chapter 33. Electromagnetic Waves What is Physics? Maxwell's Rainbow The Traveling Electromagnetic Wave, Qualitatively The Traveling.
W13D2: Maxwell’s Equations and Electromagnetic Waves
Four equations (integral form) : Gauss’s law Gauss’s law for magnetism Faraday’s law Ampere-Maxwell law + Lorentz force Maxwell’s Equations.
29. Maxwell’s Equations & Electromagnetic Waves
Lecture 21-1 Resonance For given  peak, R, L, and C, the current amplitude I peak will be at the maximum when the impedance Z is at the minimum. Resonance.
Physics 2112 Lecture 23 Electricity & Magnetism Lecture 23, Slide 1.
Physics for Scientists and Engineers, 6e
Copyright © 2009 Pearson Education, Inc. Chapter 31 Maxwell’s Equations and Electromagnetic Waves.
Chapter 34 Electromagnetic Waves. Currents produce B Change in E produces B Currents produce B Change in E produces B Change in B produces an E charges.
Wave Motion II Sinusoidal (harmonic) waves Energy and power in sinusoidal waves.
Electromagnetic Waves Chapter 35. Electromagnetic (EM) Waves Can travel through space Radio, Microwaves, IR, Light, UV, X-rays, Gamma Rays All on the.
Electromagnetic Waves
Waves Chapter 16:Traveling waves Chapter 18:Standing waves, interference Chapter 37 & 38:Interference and diffraction of electromagnetic waves.
Chapter 34 Electromagnetic Waves and light. Electromagnetic waves in our life Microwave oven, EM wave is used to deliver energy. Radio/TV, cell phones,
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Chapter 33 Electromagnetic Waves. 33.2: Maxwell’s Rainbow: As the figure shows, we now know a wide spectrum (or range) of electromagnetic waves: Maxwell’s.
Chapter 34 (continued) The Laws of Electromagnetism Maxwell’s Equations Displacement Current Electromagnetic Radiation.
Physics 1202: Lecture 18 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, etc.
Electromagnetic Waves
Physics 1202: Lecture 17 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, etc.
Tue. Nov. 11, 2008Physics 208, Lecture 211 From last time… EM waves Inductors in circuits I? + -
Heinrich Rudolf Hertz 1857 – 1894 The first person generated and received the EM waves 1887 His experiment shows that the EM waves follow the wave.
Waves - I Chapter 16 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Thursday, April 26, 2011 PHYS 1444 – Section 02 Lecture #21 Thursday April 28, 2011 Dr. Mark Sosebee for Dr. Andrew Brandt Maxwell Equations HW9 is due.
Monday, April 16, PHYS , Spring 2007 Dr. Andrew Brandt PHYS 1444 – Section 004 Lecture #21 Monday, April 30, 2007 Dr. Andrew Brandt Maxwell’s.
Physics 102: Lecture 14, Slide 1 Electromagnetic Waves Physics 102: Lecture 14.
Chapter 4: Wave equations
1Electromagnetic Waves.  Administrative ◦ Quiz Today ◦ Review Exam Grades ◦ Review Exam  Begin Chapter 23 – Electromagnetic Waves  No 10:30 Office.
Final Exam Lectures EM Waves and Optics. Electromagnetic Spectrum.
Lecture 37: FRI 19 NOV Ch.33 Electromagnetic Waves I Heinrich Hertz (1857–1894) Physics 2113 Jonathan Dowling.
Lecture 21-1 Maxwell’s Equations (so far) Gauss’s law Gauss’ law for magnetism Faraday’s lawAmpere’s law *
Today’s agenda: Electromagnetic Waves. Energy Carried by Electromagnetic Waves. Momentum and Radiation Pressure of an Electromagnetic Wave.
Q32.1 Maxwell’s equations are shown here for a region of space with no charges and no conduction currents. Complete the sentence: “The _______ equation.
Exam 3: Tuesday, April 18, 5:00-6:00 PM
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?
Electromagnetic Waves
Electromagnetic Waves
E or B? It Depends on Your Perspective
The Earth is {image} meters from the sun
Q32.1 Maxwell’s equations are shown here for a region of space with no charges and no conduction currents. Complete the sentence: “The _______ equation.
Electromagnetic waves
Electromagnetic Waves
Today’s agenda: Electromagnetic Waves.
Is charge moving?.
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 (so far)
Chapter 22 Electromagnetic Waves
Exam is Tuesday Nov. 25th in class
Presentation transcript:

P Workshop: Using Visualization in Teaching Introductory E&M AAPT National Summer Meeting, Edmonton, Alberta, Canada. Organizers: John Belcher, Peter Dourmashkin, Carolann Koleci, Sahana Murthy

P MIT Class: Electromagnetic Waves

P Maxwell’s Equations 0 0 Solve in free space (no charge/current) to get…

P Electromagnetic Radiation

P A Question of Time…

P Electromagnetic Waves: Plane Waves

P Traveling Waves Consider f(x) = x=0 What is g(x,t) = f(x-vt)? x=0 t=0 x=vt 0 t=t 0 x=2vt 0 t=2t 0 f(x-vt) is traveling wave moving to the right!

P Traveling Sine Wave: Space Look at t = 0: g(x,0) = y = y 0 sin(kx): x Amplitude (y 0 ) What is g(x,t) = f(x+vt)? Travels to left at velocity v y = y 0 sin(k(x+vt)) = y 0 sin(kx+kvt)

P Traveling Sine Wave: Time Amplitude (y 0 ) Look at x=0:

P Traveling Sine Wave

P Electromagnetic Waves Remember: Hz

P Electromagnetic Radiation: Plane Waves Watch 2 Ways: 1) Sine wave traveling to right (+x) 2)Collection of out of phase oscillators (watch one position) Don’t confuse vectors with heights – they are magnitudes of E (gold) and B (blue)

P Traveling EM Wave: Space At a fixed time (e.g. t=0): x Amplitude (E 0 )

P Traveling EM Wave: Time Amplitude (E 0 ) At x=0, just a function of time:

P Traveling E & B Waves

P PRS Question: Wave

P PRS: Wave The graph shows a plot of the function y = cos(k x). The value of k is (m) :00 1.½ m -1 2.¼ m -1  m -1  /2 m -1 5.I don’t know

P PRS Answer: Wave = 4 m  k = 2  / =  /2 m -1 y = cos (  x /2) is 1 at x = –4 m, 0 m, 4 m, etc. Answer: 4. k =  /2 m -1 (m)

P Properties of EM Waves Travel (through vacuum) with speed of light At every point in the wave and any instant of time, E and B are in phase with one another, with E and B fields perpendicular to one another, and to the direction of propagation (they are transverse):

P Direction of Propagation

P PRS Question: Direction of Propagation

P PRS: Direction of Propagation The figure shows the E (yellow) and B (blue) fields of a plane wave. This wave is propagating in the 0 1.+x direction 2.–x direction 3.+z direction 4.–z direction 5.I don’t know

P PRS Answer: Propagation The propagation direction is given by the direction of E x B (Yellow x Blue) Answer: 4. The wave is moving in the –z direction

P PRS Questions: Traveling Wave

P PRS: Traveling Wave The B field of a plane EM wave is The electric field of this wave is given by I don’t know :20

P PRS Answer: Traveling Wave From the argument of the sin(ky -  t), we know the wave propagates in the +y direction. Answer: 4.

P Group Problem: Plane Waves 1)Plot E, B at each of the ten points pictured for t=0 2)Why is this a “plane wave?”

P Electromagnetic Radiation Both E & B travel like waves: But there are strict relations between them: Here, E y and B z are “the same,” traveling along x axis

P Amplitudes of E & B E y and B z are “the same,” just different amplitudes

P Electromagnetic Radiation: Plane Waves

P How Do Maxwell’s Equations Lead to EM Waves? Derive Wave Equation Optional

P Wave Equation Start with Ampere-Maxwell Eq:

P Wave Equation So in the limit that dx is very small: Apply it to red rectangle: Start with Ampere-Maxwell Eq:

P Wave Equation Now go to Faraday’s Law

P Wave Equation Faraday’s Law: So in the limit that dx is very small: Apply it to red rectangle:

P D Wave Equation for E Take x-derivative of 1st and use the 2nd equation

P D Wave Equation for E This is an equation for a wave. Let:

P D Wave Equation for B Take x-derivative of 1st and use the 2nd equation

P Electromagnetic Waves Both E & B travel like waves: But there are strict relations between them: Here, E y and B z are “the same,” traveling along x axis

P Energy in EM Waves Energy densities: Consider cylinder: What is rate of energy flow per unit area?

P Poynting Vector and Intensity units: Joules per square meter per sec Direction of energy flow = direction of wave propagation Intensity I:

P Momentum & Radiation Pressure EM waves transport energy: This is only for hitting an absorbing surface. For hitting a perfectly reflecting surface the values are doubled: They also transport momentum: And exert a pressure:

P Standing Waves

P Standing Waves What happens if two waves headed in opposite directions are allowed to interfere?

P Standing Waves Most commonly seen in resonating systems: Musical Instruments, Microwave Ovens

P Group Work: Standing Waves

P Generating Plane Electromagnetic Radiation

P30 - Shake a Sheet of Charge generating plane wave radiationgenerating plane wave radiation applet

P30 - 2) If sheet position is What is B(x,t)? What is E(x,t)? What Direction? Group Problem: B Field Generation Sheet (blue) has uniform charge density  Starting time T ago pulled down at velocity v 1) What is B field? (HINT: Change drawing perspective) sheet

P30 - You Made a Plane Wave! generating plane wave

P30 - How to Think About E-Field E-Field lines like strings tied to plane This is the field you calculated & that propagates

P Group Problem: Energy in Wave You Found: 1) What is total power per unit area radiated away? 2) Where is that energy coming from? 3) Calculate power generated to see efficiency

P Generating Electric Dipole Electromagnetic Waves

P30 - Quarter-Wavelength Antenna Accelerated charges are the source of EM waves. Most common example: Electric Dipole Radiation. t = 0t = T/4t = T/2t = T

P30 - Why are Radio Towers Tall? AM Radio stations have frequencies 535 – 1605 kHz. WLW 700 Cincinnati is at 700 kHz. Tower is 747 ft tall

P30 - Quarter-Wavelength Antenna

P30 - Quarter-Wavelength Antenna

P30 - Spark Gap Transmitter

P Spark Gap Generator: An LC Oscillator

P Our spark gap antenna 1) Charge gap (RC) 2) Breakdown! (LC) 3) Repeat

P30 - Spark Gap Transmitter

P30 - PRS Question: Spark Gap Antenna

P30 - Spark Gap Antenna

P30 - Spark Gap Antenna

P30 - Demonstration: Antenna

P30 - Polarization

P30 - Polarization of TV EM Waves Why oriented as shown? Why different lengths?

P30 - Demonstration: Microwave Polarization

P30 - Experiment 8: Microwaves

P30 - Standing Waves What happens if two waves headed in opposite directions are allowed to interfere?

P30 - PRS Questions: Angular Distribution & Polarization of Radiation