Lecture 34: MON 13 APR Ch ,5

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1 Physics 2102 Jonathan Dowling James Clerk Maxwell ( ) Lecture 34: MON 13 APR Ch ,5 3,5 7: E&M Waves

2 MT03 Avg: 65/100 Q1/P3 K. Schafer Office hours: MW 1:30-2:30 pm 222B Nicholson P1/Q2 J. Dowling Office hours: MWF 10:30-11:30 am 453 Nicholson P2/Q3 M. Gaarde Office hours: TTh 2:30-3:30 pm 215B Nicholson P3/Q2 C. Buth Office hours: MF 2:30-3:30 pm 222A Nicholson A: B: C: D: 50-59

3 Problem 1 [18 points] In the figure below, two semicircular arcs (I & II) have radii R 1 = 4.10 cm and R 2 = 6.60 cm, carry current i = A, and share the same center of curvature C. The same current i also flows through the straight sections of wire labeled III & IV. (a) (5 pts) What is the contribution to the magnitude of the magnetic field at point C from the two straight sections of wire III and IV? Explain your answer! Question 2 [8 points] The figure below shows four arrangements in which long parallel wires carry equal currents i directly into or out of the page at the corners of identical squares. B III = B IV = 0 d! B! d! s "! r = 0 Biot-Savart (b) (8 pts) Calculate the magnitude of the magnetic field at the point C due to all four sections of wire. (i) (4 pts) For square B, what is the direction of the magnetic field, with respect to the page, at the center of the square? Circle one: B TOT = B! I! B! II = µ 0i" $ 4# % & " = # = half a circle 1! 1 ' R I R II ( ) = 8.14 * 10!7 T Out ( ) In! Up " Down# Left $ Right % Field is Zero ( B! = 0) Right Hand Rule & Vector Addition! Right Hand Rule & B I >B II Since I is Closer! (c) (5 pts) What is the direction of the total magnetic field at the point C due to all four sections of wire? Circle one: Out of the page ( ). Into the page. Up towards the top of the page. Down towards the bottom of the page. To the right of the page. To the left of the page. The total magnetic field at C is zero and has no direction. (ii) (4 pts) Rank the sections according to the magnitude of the magnitude of the magnetic field at the center of each square, greatest first. Circle one: B A > B B > B C B C > B B > B A B A > B C > B B B B > B C > B A B A = B B = B C B= µ 0 i 2!r!;!!!!!!B A = 0;!!!!!B B = 2 2B;!!!!!B C = 2B;

4 Maxwell, Waves and Light A solution to the Maxwell equations in empty space is a traveling wave! B ds = µ 0 "! 0 E C d dt S da! E ds = "! B C d dt S da electric and magnetic forces can travel! d 2 E dx 2 =!µ 0" 0 d 2 E dt 2 # E = E 0 sin k(x! ct) c = 1 µ 0! 0 = 3 " 10 8 m/s The electric waves travel at the speed of light! Light itself is a wave of electricity and magnetism!

5 Electromagnetic Waves A solution to Maxwell s equations in free space: E = E sin( kx "! t) m B = B sin( kx "! t) m! k = c, speed of propagation. c = E m B m = 1 µ 0! 0 =299,462,954 m s!=!187,163 miles/sec Visible light, infrared, ultraviolet, radio waves, X rays, Gamma rays are all electromagnetic waves.

8 Radio waves are reflected by the layer of the Earth s atmosphere called the ionosphere. This allows for transmission between two points which are far from each other on the globe, despite the curvature of the earth. Marconi s experiment discovered the ionosphere! Experts thought he was crazy and this would never work.

$visible is only a tiny fraction of the entire electromagnetic spectrum. Fig. 33-2 Fig.$

9 Maxwell s Rainbow The wavelength/frequency range in which electromagnetic (EM) waves (light) are visible is only a tiny fraction of the entire electromagnetic spectrum. Fig Fig (33-2)

10 The Traveling Electromagnetic (EM) Wave, Qualitatively An LC oscillator causes currents to flow sinusoidally, which in turn produces oscillating electric and magnetic fields, which then propagate through space as EM waves. Next slide Fig Oscillation Frequency:! = 1 LC (33-3)

11 Mathematical Description of Traveling EM Waves Electric Field: E = E ( kx "! t) m sin Magnetic Field: B = B ( kx "! t) m sin Wave Speed: c = 1 µ! 0 0 All EM waves travel a c in vacuum EM Wave Simulation Wavenumber: k = 2! " = # c Frequency:! = 2" T = 2" f Vacuum Permittivity:! 0 Vacuum Permeability: µ 0 Fig Amplitude Ratio: Em c B = E ( t) Magnitude Ratio: m B( t) = c (33-5)

12 The Poynting Vector: Points in Direction of Power Flow Electromagnetic waves are able to transport energy from transmitter to receiver (example: from the Sun to our skin). The power transported by the wave and its direction is quantified by the Poynting vector. John Henry Poynting ( )! S = 1 µ 0! E!! B For a wave, since E is perpendicular to B: Units: Watt/m 2 B E S 1 1 S = EB = E µ cµ In a wave, the fields change with time. Therefore the Poynting vector changes too!! 0 The direction is constant, but the magnitude changes from 0 to a maximum value. 0 2

EM Wave Intensity, Energy Density A better measure of the amount of energy in an EM wave is obtained by averaging the Poynting vector over one wave cycle. The resulting quantity is called intensity.

13 EM Wave Intensity, Energy Density A better measure of the amount of energy in an EM wave is obtained by averaging the Poynting vector over one wave cycle. The resulting quantity is called intensity. Units are also Watts/m 2. I = S = 1 cµ 0 I E 2 = 1 E 2 m sin 2 (kx! "t) cµ 0 = 1 2cµ 0 2 E m or, I = 1 The average of sin E 2 over m 2cµ one cycle is ½: 0 1 c = µ0 2 E rms E m 2 2 E rms Both fields have the same energy density B 1 B ue =! 0E =! 0( cb) =! 0 = = ub 2 2 2! 0 µ 0 2 µ 0 The total EM energy density is then u =! = B E / µ 0

P = IA = (10 3 W/m 2 ) x 8m x 20m = 0.16 MegaWatt!! The solar panel shown (BP- 275) has dimensions 47in x 29in.

14 Solar Energy The light from the sun has an intensity of about 1kW/m 2. What would be the total power incident on a roof of dimensions 8m x 20m? I = 1kW/m 2 is power per unit area. P = IA = (10 3 W/m 2 ) x 8m x 20m = 0.16 MegaWatt!! The solar panel shown (BP- 275) has dimensions 47in x 29in. The incident power is then 880 W. The actual solar panel delivers 75W (4.45A at 17V): less than 10% efficiency. The electric meter on a solar home runs backwards Entergy Pays YOU!

EM Spherical Waves The intensity of a wave is power per

pierces a larger and larger sphere as the wave travels

15 EM Spherical Waves The intensity of a wave is power per unit area. If one has a source that emits isotropically (equally in all directions) the power emitted by the source pierces a larger and larger sphere as the wave travels outwards: 1/r 2 Law! I = P s 4! r 2 So the power per unit area decreases as the inverse of distance squared.

and the energy incident normally on a square plate of side 10cm in 5 minutes. P s 4!r = 10kW 2 4!

16 I = Example A radio station transmits a 10 kw signal at a frequency of 100 MHz. At a distance of 1km from the antenna, find the amplitude of the electric and magnetic field strengths, and the energy incident normally on a square plate of side 10cm in 5 minutes. P s 4!r = 10kW 2 4!(1km) = 2 0.8mW/m2 I = 1 E 2 m! E m = 2cµ 0 I = 0.775V/m 2cµ 0 B m = E m / c = 2.58nT Received energy: S = P A =!U /t A "!U = SAt = 2.4 mj

17 Radiation Pressure Waves not only carry energy but also momentum. The effect is very small (we don t ordinarily feel pressure from light). If light is completely absorbed during an interval Dt, the momentum transferred is given by! u and twice as much if reflected. Newton s law: F =! p =! p! t Now, supposing one has a wave that hits a surface of area A (perpendicularly), the amount of energy transferred to that surface in time Dt will be! U = IA! t therefore Radiation pressure: c! p = IA! t c p r = I c (total absorption), p r = 2I c I F = (total reflection) IA c A F [N/m 2 ]

18 Radiation Pressure & Comet Tails

19 Solar Sails: Photons Propel Spacecraft! StarTrek DS9 NASA Concept NASA Demo

20 Radio transmitter: EM waves: polarization If the dipole antenna is vertical, so will be the electric fields. The magnetic field will be horizontal. The radio wave generated is said to be polarized. In general light sources produce unpolarized waves emitted by atomic motions in random directions.

Therefore running the light through a polarizer will cut the intensity in half: I=I 0 /2

21 EM Waves: Polarization Completely unpolarized light will have equal components in horizontal and vertical directions. Therefore running the light through a polarizer will cut the intensity in half: I=I 0 /2 When polarized light hits a polarizing sheet, only the component of the field aligned with the sheet will get through. E y = E cos(! ) And therefore: I = I 2 0 cos!

$Example Initially unpolarized light of intensity I 0 is sent into a system of three polarizers as shown. What fraction of the initial intensity emerges from the system?$

22 Example Initially unpolarized light of intensity I 0 is sent into a system of three polarizers as shown. What fraction of the initial intensity emerges from the system? What is the polarization of the exiting light? Through the first polarizer: unpolarized to polarized, so I 1 =½I 0. Into the second polarizer, the light is now vertically polarized. Then, I 2 = I 1 cos 2 60 o = 1/4 I 1 = 1/8 I 0. Now the light is again polarized, but at 60o. The last polarizer is horizontal, so I 3 = I 2 cos 2 30 o = 3/4 I 2 =3 /32 I 0 = I 0. The exiting light is horizontally polarized, and has 9% of the original amplitude.

Lecture 38: FRI 24 APR Ch.33 Electromagnetic Waves

Physics 2113 Jonathan Dowling Heinrich Hertz (1857 1894) Lecture 38: FRI 24 APR Ch.33 Electromagnetic Waves Maxwell Equations in Empty Space: E da = 0 S B da = 0 S C C B ds = µ ε 0 0 E ds = d dt d dt S