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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

Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

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Page 1: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

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

Page 2: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

Electromagnetic Waves

Page 3: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

Eye Sensitivity to Color

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Production of Electromagnetic waves

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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 6: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

Electromagnetic Wave

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Page 8: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

Wave Equation

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How the fields

vary at a Point

P in space as

the wave goes

by

Page 12: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

Spherical waves Plane waves

Page 13: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

A point source of light generates a spherical wave. Light is

emitted isotropically and the intensity of it falls off as 1/r2

Let P be the power of the source

in joules per sec. Then the intensity

of light at a distance r is

24 r

PI

!=

What do we mean by Intensity of

light?

Spherical Waves

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17. The maximum electric field at a distance of 10 m from an isotropic

point 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 $

V

m( ) 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=!==

"##

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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 22: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

Polarization of light

Resolved into its y and z-components The sum of the y-components and z components are equalPass though a polarizing sheet

aligned to pass only the y-component

Page 23: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

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

Intensity I0

One Half Rule

Half the intensity out

I =I0

2

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I2= I

1cos

2!

I0

I1=I0

2

I ! Ey

2

Ey= E cos"

y

Page 26: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

35. In the figure, initially unpolarized light is sent through three

polarizing sheets whose polarizing directions make angles of !1 = 40o,

!2 = 20o, and !3 = 40o with the direction of the y axis. What percentage

of the light’s initial intensity is transmitted by the system? (Hint: Be

careful with the angles.)

Let Io be the intensity of the unpolarized light that

is incident on the first polarizing sheet. The

transmitted intensity of is I1 = (1/2)I0, and the

direction of polarization of the transmitted light is

!1 = 40o counterclockwise from the y axis in the

diagram. The polarizing direction of the second

sheet is !2 = 20o clockwise from the y axis, so the

angle between the direction of polarization that is

incident on that sheet and the the polarizing

direction of the sheet is 40o + 20o = 60o. The

transmitted intensity is

,60cos2

160cos

2

0

2

12

ooIII ==

and the direction of polarization of the transmitted light is 20o clockwise

from the y axis.

I1

I2

I3

I0

Page 27: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

35. In the figure, initially unpolarized light is sent through three

polarizing sheets whose polarizing directions make angles of !1 = 40o,

!2 = 20o, and !3 = 40o with the direction of the y axis. What percentage

of the light’s initial intensity is transmitted by the system? (Hint: Be

careful with the angles.)

The polarizing direction of the third sheet is !3

= 40o counterclockwise from the y axis.

Consequently, the angle between the

direction of polarization of the light incident on

that sheet and the polarizing direction of the

sheet is 20o + 40o = 60o. The transmitted

intensity 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 28: Lecture 13 Electromagnetic Waves Ch. 33 - Galileogalileo.phys.virginia.edu/classes/632.ral5q.summer... · Lecture 13 Electromagnetic Waves Ch. 33 ¥Cartoon ¥Opening Demo ¥Topics

Polarization can be produced by:• Scattering• Reflection

Light scattered from sky is partially polarizedLight scattered from your car hood is polarizedin the plane of the hood.

See Brewsters Law

Light is also refracted when changing mediums