1 my chapter 22 lecture. 2 chapter 22: electromagnetic waves production of em waves maxwell’s...

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1 My Chapter 22 Lecture

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Page 1: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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MyChapter 22

Lecture

Page 2: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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Chapter 22: Electromagnetic Waves

•Production of EM waves

•Maxwell’s Equations

•Antennae

•The EM Spectrum

•Speed of EM Waves

•Doppler Effect

Page 3: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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§22.1 Maxwell’s Equations and EM Waves

A stationary charge produces an electric field.

A charge moving at constant speed produces electric and magnetic fields.

Page 4: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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A charge that is accelerated will produce variable electric and magnetic fields. These are electromagnetic (EM) waves.

If the charge oscillates with a frequency f, then the resulting EM wave will have a frequency f. If the charge ceases to oscillate, then the EM wave is a pulse (a finite-sized wave).

Page 5: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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Faraday’s Law:

A changing magnetic field creates an electric field.

Ampère-Maxwell Law

A current or a changing electric field creates a magnetic field.

Page 6: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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When Maxwell’s equations are combined, the solutions are electric and magnetic fields that vary with position and time. These are EM waves.

An electric field only wave cannot exist, nor can a magnetic field only wave.

Page 7: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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§22.2 Antennae

An electric field parallel to an antenna (electric dipole) will “shake” electrons and produce an AC current.

Page 8: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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An EM wave also has a magnetic component. A magnetic dipole antenna can be oriented so that the B-field passes into and out of the plane of a loop, inducing a current in the loop.

The B-field of an EM wave is perpendicular to its E-field and also the direction of travel.

Page 9: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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§22.3 The EM Spectrum

EM waves of any frequency can exist.

Page 10: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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The EM Spectrum:

Energy increases with increasing frequency.

Page 11: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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§22.4 Speed of Light

Maxwell was able to derive the speed of EM waves in vacuum. EM waves do not need a medium to travel through.

( )( )m/s 1000.3

Tm/A 104/NmC 1085.8

1

1

8

72212

00

×=

××=

=

−− π

μεc

Page 12: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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In 1675 Ole Römer presented a calculation of the speed of light. He used the time between eclipses of Jupiter’s Gallilean Satellites to show that the speed of light was finite and that its value was 2.25108 m/s.

Fizeau’s experiment of 1849 measured the value to be about 3108 m/s. (done before Maxwell’s work)

Page 13: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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When light travels though a material medium, its speed is reduced.

n

cv =

where v is the speed of light in the medium and n is the refractive index of the medium.

When a wave passes from one medium to another the frequency stays the same, but the wavelength is changed.

A dispersive medium is one in which the index of refraction depends on the wavelength of light.

Page 14: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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Example (text problem 22.22): In order to study the structure of a crystalline solid, you want to illuminate it with EM radiation whose wavelength is the same as the spacing of the atoms in the crystal (0.20 nm).

(a) What is the frequency of the EM radiation?

(b) In what part of the EM spectrum does it lie?

Hz 105.1m 1020.0

m/s 100.3 159

8

×=×

×== −λ

cf

X-ray

Page 15: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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§22.5 Properties of EM Waves

All EM waves in vacuum travel at the “speed of light” c.

Both the electric and magnetic fields have the same oscillation frequency f.

The electric and magnetic fields oscillate in phase.

Page 16: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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The fields are related by the relationship

),,,(),,,( tzyxcBtzyxE =

EM waves are transverse. The fields oscillate in a direction that is perpendicular to the wave’s direction of travel. The fields are also perpendicular to each other.

Page 17: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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The direction of propagation is given by .BE×

The wave carries one-half of its energy in its electric field and one-half in its magnetic field.

Page 18: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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§22.8 The Doppler Effect

cvcv

ff so

+=

1

1For EM waves, the Doppler shift formula is

where fs is the frequency emitted by the source, fo is the frequency received by the observer, v is the relative velocity of the source and the observer, and c is the speed of light.

Page 19: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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When v/c << 1, the previous expression can be approximated as:

⎟⎠

⎞⎜⎝

⎛ +≈c

vff so 1

If the source and observer are approaching each other, then v is positive, and v is negative if they are receding.

Page 20: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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Example (text problem 22.56): Light of wavelength 659.6 nm is emitted by a star. The wavelength of this light as measured on Earth is 661.1 nm. How fast is the star moving with respect to the Earth? Is it moving toward Earth or away from it?

The wavelength shift is small (λ << λ) so v << c.

km/s 680m/s 108.6

0023.011/

/1

1

5 −=×−=

−=−=−=−=

⎟⎠

⎞⎜⎝

⎛ +≈

v

cc

ff

cv

cv

ff

o

s

s

o

s

o

so

λλ

λλ

Star is receding.

Page 21: 1 My Chapter 22 Lecture. 2 Chapter 22: Electromagnetic Waves Production of EM waves Maxwell’s Equations Antennae The EM Spectrum Speed of EM Waves Doppler

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Summary

•Maxwell’s Equations

•Electric and Magnetic Dipole Antennae

•EM Spectrum

•Properties of EM Waves

•Doppler Effect