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Electromagnetic Waves

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Page 1: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Electromagnetic Waves

Page 2: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Lecture 13 Electromagnetic Waves Ch. 33

• Cartoon• Opening Demo• Topics

– Electromagnetic waves– Traveling E/M wave - Induced electric and induced magnetic amplitudes– Plane waves and spherical waves– Energy transport Poynting vector– Pressure produced by E/M wave– Polarization– Reflection, refraction,Snell’s Law, Internal reflection– Prisms and chromatic dispersion– Polarization by reflection-Brewsters angle

• Elmo• Polling

Page 3: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Electromagnetic Waves

Page 4: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Eye Sensitivity to Color

Page 5: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Production of Electromagnetic waves

Page 6: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Spherical waves Plane waves

Page 7: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

To investigate further the properties of electromagnetic waves we consider the simplest situation of a plane wave. A single wire with variable current generates propagating electric and magnetic fields with cylindrical symmetry around the wire.

If we now stack several wires parallel to each other, and make this stack wide enough (and the wires very close together), we will have a (plane) wave propagating in the z direction, with E-field oriented along x, E = Ex (the current direction) and B-field along y B=By (Transverse waves)

Page 8: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Electromagnetic Wave

Page 9: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

How the fieldsvary at a PointP in space as

the wave goesby

Page 10: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening
Page 11: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Electromagnetic Wave

Page 12: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Electromagnetic Wave Self Generation

• Faraday’s Law ofInduction

• Maxwell’s Law ofInduction

• Changing electric fieldinduces a magneticfield

• Changing magneticfield induces a electricfield

!E.d!s = !

d"B

dx"#

!B.d!s = µ

0!0

d"E

dx"#c =

1

µ0!0

Page 13: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Summary

Page 14: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

!S =

dU

Adt

U is the energy carried by a wave

Magnitude of S is like the intensity

Page 15: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

S =dU

Adt

Page 16: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

B0=E0

c

Page 17: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

A point source of light generates a spherical wave. Light isemitted isotropically and the intensity of it falls off as 1/r2

Let P be the power of the sourcein joules per sec. Then the intensity of light at a distance r is

24 r

PI

!=

Lets look at an example

Relation of intensity and power for a Spherical Wave

Page 18: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

15 . The maximum electric field at a distance of 10 m from an isotropicpoint light source is 2.0 V/m. Calculate

(a) the maximum value of the magnetic field and

(b) the average intensity of the light there?

(c) What is the power of the source?

(a) The magnetic field amplitude of the wave is

Tc

EB

s

m

m

V

m

m

9

8107.6

10998.2

0.2!

"="

==

(b) The average intensity is

Iavg =E2

m

2µ0c=

2.0V

m( )2

2 4! "10#7T $

m

A( ) 2.998 "108 m

s( )= 5.3"10#3 W

m2

(c) The power of the source is

( ) ( ) WmIrPm

Wavg 7.6103.51044

2

322=!==

"##

Page 19: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening
Page 20: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Speed of light in Water v =c

n=2.998 !10

8 m

s

1.33= 2.26 !10

8 m

s

Page 21: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Nothing is known to travel faster than light in a vacuum

However, electrons can travel faster than light in water.And when the do the electrons emit light called Cerenkov radiation

Page 22: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening
Page 23: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Momentum and Radiation Pressure

c

Momentum = p

p=U/c paper

Light beam

1) Black paper absorbs all the light

p=0!p = !U / c

What is the change in momentum of thepaper over some time interval?

2) Suppose light is 100% reflected

!p = p " (" p) = 2p !p = 2!U / c

From this we define the pressure

Page 24: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Radiation Pressure Pr

Want to relate the pressure Pr felt by the paper to the intensity of light

I =Power

Area=!U / !t

A

Pr =F

A=!p / !t

A

!p = !U / c For 100% absorption of light on the paper

Pr=F

A=c!U / !t

A= cI

Pr=F

A=2c!U / !t

A= 2cI For 100% reflection of light

Page 25: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Problem 21What is the radiation pressure 1.5 m away from a 500Watt lightbulb?

Page 26: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Radiation pressure: Light carries momentum

Pr

=I

c

This is the force per unit area felt by an object that absorbs light. (Black piece of paper))

Pr

=2I

c

This is the force per unit area felt by an object that reflects light backwards. (Aluminum foil)

Another property of light

Page 27: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Polarization of Light

• All we mean by polarization is whichdirection is the electric vector vibrating.

• If there is no preferred direction the wave isunpolarized

• If the preferred direction is vertical, then wesay the wave is vertically polarized

Page 28: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Pass though a polarizing sheet aligned to pass only the y-component

A polarizing sheet or polaroid filter is specialmaterial made up of rows ofmolecules that only allow light to pass when the electricvector is in one direction.

Page 29: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Resolved into its y and z-components The sum of the y-components and z components are equal

Unpolarized light

Page 30: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Pass though a polarizing sheet aligned to pass only the y-componentMalus’s Law

Intensity I0

One Half RuleHalf the intensity out

I =I0

2

Page 31: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

I2= I

1cos

2!

I0

I1=I0

2

I ! Ey

2

Ey= E cos"

E2

y= E

2cos

2"

I2= I

1cos

2"

y

Ey= E cos!

Polarizer P1

Analyzer P2

Page 32: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Sunglasses are polarized vertically.Light reflected from sky is partially polarizedand light reflected from car hoods is polarizedin the plane of the hood

Sunglass 1

Sunglass 2

Rotate sun glass 90 deg and no light gets through because cos 90 = 0

Page 33: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

35. In the figure, initially unpolarized light is sent through threepolarizing sheets whose polarizing directions make angles of θ1 = 40o,θ2 = 20o, and θ3 = 40o with the direction of the y axis. What percentageof the light’s initial intensity is transmitted by the system? (Hint: Becareful with the angles.)

Let Io be the intensity of the unpolarized light thatis incident on the first polarizing sheet. Thetransmitted intensity of is I1 = (1/2)I0, and thedirection of polarization of the transmitted light is θ1 = 40o counterclockwise from the y axis in thediagram. The polarizing direction of the secondsheet is θ2 = 20o clockwise from the y axis, so theangle between the direction of polarization that isincident on that sheet and the the polarizingdirection of the sheet is 40o + 20o = 60o. Thetransmitted intensity is

,60cos2

160cos

2

0

2

12

ooIII ==

and the direction of polarization of the transmitted light is 20o clockwisefrom the y axis.

I1

I2

I3

I0

Page 34: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

35. In the figure, initially unpolarized light is sent through threepolarizing sheets whose polarizing directions make angles of θ1 = 40o,θ2 = 20o, and θ3 = 40o with the direction of the y axis. What percentageof the light’s initial intensity is transmitted by the system? (Hint: Becareful with the angles.)

The polarizing direction of the third sheet is θ3= 40o counterclockwise from the y axis.Consequently, the angle between thedirection of polarization of the light incident onthat sheet and the polarizing direction of thesheet is 20o + 40o = 60o. The transmittedintensity is

I3= I

2cos

260

o

I2= I

1cos

260

o

I1=1

2I0

I3

I0

=1

2cos

460 = 3.125 !10

"2

Thus, 3.1% of the light’s

initial intensity is transmitted.

Page 35: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Chapter 33 Problem 34In Figure 33-42, initially unpolarized light is sent into a system ofthree polarizing sheets whose polarizing directions make angles ofθ1 = θ2 = θ3 = 16° with the direction of the y axis. Whatpercentage of the initial intensity is transmitted by the system?

Fig. 33-42

Page 36: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Chapter 33 Problem 49

In Figure 33-51, a 2.00 m long vertical pole extends from thebottom of a swimming pool to a point 90.0 cm above thewater. Sunlight is incident at angle θ = 55.0°. What is thelength of the shadow of the pole on the level bottom of thepool?

Fig. 33-51

Page 37: PHYS632 L13 ch 33 Ele Waves 08 - people.Virginia.EDUpeople.virginia.edu/~ral5q/classes/phys632/summer08/Lecture1-16... · Lecture 13 Electromagnetic Waves Ch. 33 •Cartoon •Opening

Chapter 33 Problem 62 Suppose the prism of Figure 33-55 has apex angle ϕ = 69.0° and index of

refraction n = 1.59.

Fig. 33-55(a) What is the smallest angle of incidence θ for which a ray can enter the

left face of the prism and exit the right face?(b) What angle of incidence θ is required for the ray to exit the prism with

an identical angle θ for its refraction, as it does in Figure 33-55?

In Figure 33-51, a 2.00 m long vertical pole extends from the bottom of aswimming pool to a point 90.0 cm above the water. Sunlight isincident at angle θ = 55.0°. What is the length of the shadow of thepole on the level bottom of the pool?