Review: Basic Concepts

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1 Review: Basic Concepts Simula5ons 1. Radio Waves h;p://phet.colorado.edu/en/simula5on/radio- waves 2. Propaga5on of EM Waves h;p:// 3. 2D EM Waves h;p://

2 Maxwell s Equa,ons

3 The Fundamental Ideas of Electromagne,sm

Electromagne,c Waves Maxwell, using his equa5ons of the electromagne5c field, was the first to understand that light is an oscilla5on of the electromagne5c field.

4 Electromagne,c Waves Maxwell, using his equa5ons of the electromagne5c field, was the first to understand that light is an oscilla5on of the electromagne5c field. Maxwell was able to predict that Electromagne5c waves can exist at any frequency, not just at the frequencies of visible light. This predic5on was the harbinger of radio waves. All electromagne5c waves travel in a vacuum with the same speed, a speed that we now call the speed of light.

6 Proper,es of Electromagne,c Waves Any electromagne5c wave must sa5sfy four basic condi5ons: 1. The fields E and B and are perpendicular to the direction of propagation v em.thus an electromagnetic wave is a transverse wave. 2. E and B are perpendicular to each other in a manner such that E B is in the direction of v em. 3. The wave travels in vacuum at speed v em = c 4. E = cb at any point on the wave.

7 Proper,es of Electromagne,c Waves The energy flow of an electromagne5c wave is described by the Poyn,ng vector defined as The magnitude of the Poyn5ng vector is The intensity of an electromagne5c wave whose electric field amplitude is E 0 is

8 EXAMPLE: The electric field of a laser beam

Radia,on Pressure It s interes5ng to consider the force of an electromagne5c wave exerted on an object per unit area, which is called the radia,on pressure p rad.

9 Radia,on Pressure It s interes5ng to consider the force of an electromagne5c wave exerted on an object per unit area, which is called the radia,on pressure p rad. The radia5on pressure on an object that absorbs all the light is energy absorbed Δp = c F = Δp energy absorbed = Δt c ( E = pc) ( ) / Δt = P c where P is the power (joules per second) of the light. where I is the intensity of the light wave. The subscript on p rad is important in this context to dis5nguish the radia5on pressure from the momentum p.

10 Example Solar sailing

11 Polariza5on & Plane of Polariza5on

12 A Polarizing Filter

13 Malus s Law Suppose a polarized light wave of intensity I 0 approaches a polarizing filter. θ is the angle between the incident plane of polariza5on and the polarizer axis. The transmi;ed intensity is given by Malus s Law: If the light incident on a polarizing filter is unpolarized, the transmi;ed intensity is In other words, a polarizing filter passes 50% of unpolarized light and blocks 50%.

14 Intermediate/Advanced Concepts

15 Wave equa5ons in a medium The induced polariza5on in Maxwell s Equa5ons yields another term in the wave equa5on: E z E t 2 2 µε = E 1 E = z v t This is the Inhomogeneous Wave Equa,on. The polariza5on is the driving term for a new solu5on to this equa5on. E z E t 2 2 µε = E 1 E = z c t Homogeneous (Vacuum) Wave Equa,on 0 E ( zt) ikz ( ωt), = Re{ E e } = + 0 ikz ( ωt) * ikz ( ωt) { E e E e } ( kz ωt) = E cos n 2 2 c = = 2 v µε µε 0 0 c v = n

16 Propaga5on of EM Waves

17 Polariza5on and Propaga5on

18 Energy and Intensity S=E H Poyn,ng vector describes flows of E- M power Power flow is directed along this vector (usually parallel to k) Intensity is average energy transfer (i.e. the 5me averaged Poyning vector: I=<S>=P/A, where P is the power (energy transferred per second) of a wave that impinges on area A. sin 2 ( kx ωt) = cos 2 ( kx ωt) = 1 2 cε cε S = I E t H t = E = E + E x cε A/ V 0 example E = 1 V / m ( ) ( ) ( 2 2) I =? W / m y hω[ ev ] = λ[ nm] h = Js

19 Linear polariza5on (frozen 5me)

20 Linear polariza5on (fixed space)

21 Circular polariza5on (linear components)

22 Circular polariza5on (frozen 5me)

23 Circular polariza5on (fixed space)

24 Linear versus Circular Polariza5on

25 Methods for genera5ng polarized light h;p://hyperphysics.phy- astr.gsu.edu/hbase/phyopt/polar.html

26 Polariza5on by Reflec5on h;p://hyperphysics.phy- astr.gsu.edu/hbase/phyopt/polar.html

27 Malus s Law

28 Where is the turtle?

29 Polarized sunglasses

30 Brewster Angle

31 Polariza5on by sca;ering (Rayleigh sca;ering/blue Sky)

32 Circularly polarized light in nature

33 Morphology and microstructure of cellular pa;ern of C. gloriosa

34 Quarter wave plate

35 Half wave plate

36 Quiz for the Lab Bonus Credit 0.2 pts

lef ellip5cal polariza5on Phase difference = 0 0 Ex r ẑ Ex r Phase

37 ŷ E = E x e iδ 1 iδ 2 xˆ + Eye yˆ Polariza5on: Summary ŷ E xˆ xˆ linear polariza5on y- direc5on right circular polariza5on lef circular polariza5on lef ellip5cal polariza5on Phase difference = 0 0 Ex r ẑ Ex r Phase difference è 90 0 (π/2, λ/4) ẑ Ex r Phase difference è (π, λ/2) ẑ E y ẑ E y ẑ E y ẑ

38 Polariza5on Applets Polariza5on Explora5on h;p://webphysics.davidson.edu/physlet_resources/dav_op5cs/examples/polariza5on.html 3D View of Polarized Light h;p://fipsgold.physik.uni- kl.de/sofware/java/polarisa5on/index.html

39 Reflec5on and dielectric interface

40 Beyond Snell s Law: Polariza5on?

41 Reflec5on and Transmission (Fresnel s equa5ons) Can be deduced from the applica,on of boundary condi,ons of EM waves. An online calculator is available at hop://hyperphysics.phy- astr.gsu.edu/hbase/phyopt/freseq.html

42 Reflec5on and Transmission of dielectric interfaces

43 Reflec5on and Transmission (Fresnel s equa5ons) Can be deduced from the applica,on of boundary condi,ons of EM waves.

44 Reflec5on and Transmission of dielectric interfaces

45 Energy Conserva5on

46 Normal Incidence

47 Reflectance and dielectric interfaces

Electromagne,c Waves. All electromagne-c waves travel in a vacuum with the same speed, a speed that we now call the speed of light.

Electromagne,c Waves. All electromagne-c waves travel in a vacuum with the same speed, a speed that we now call the speed of light. Electromagne,c Waves All electromagne-c waves travel in a vacuum with the same speed, a speed that we now call the speed of light. Proper,es of Electromagne,c Waves Any electromagne-c wave must sa-sfy