PHY222 PHYSICAL OPTICS AND
DOPPLER EFFECT
                   by
              Mr. Y. Kalolo
Lecture 2                DOPPLER EFFECT
Table Of Contents
1. The Electromagnetic Spectrum
2. The Doppler Effect
Section 1:
The Electromagnetic Spectrum
THE ELECTROMAGNETIC SPECTRUM
THE ELECTROMAGNETIC SPECTRUM
   An electromagnetic (EM) wave, like any periodic wave, has a
    frequency f and a wavelength λ that are related to the
    speed v of the wave by v = f λ
   For EM waves travelling through a vacuum, or to a good
    approximation, through air, the speed is v = c, so c = f λ
   EM waves exist with an enormous range of frequencies,
    from values less than 104 Hz to greater than 1024 Hz
   Since all these waves travel through a vacuum at the same
    speed of c = 3.00 x 108 m/s, equation c = f λ can be used
    to find the correspondingly wide range of wavelengths.
   The ordered series of electromagnetic wave frequencies or
    wavelengths is called the electromagnetic spectrum.
THE ELECTROMAGNETIC SPECTRUM
         © Cutnell J.D. & Johnson K.W. (2010) Introduction to Physics, 8 th Ed. John Wiley & Sons Pvt Ltd
REGIONS OF THE EM SPECTRUM
   Historically, regions of the spectrum have been given names such as
    radio waves and infrared waves. Although the boundary between
    adjacent regions is shown as a sharp line in the drawing, the boundary is
    not so well defined in practice, and the regions often overlap.
   Beginning on the left in the spectrum, we find radio waves. Lower-
    frequency radio waves are generally produced by electrical oscillator
    circuits, while higher-frequency radio waves (called microwaves) are
    usually generated using electron tubes called klystrons.
   Infrared radiation (heat waves), originates with the vibration and
    rotation of molecules within a material.
   Visible light is emitted by hot objects, such as the sun, a burning log, or
    the filament of an incandescent light bulb, when the temperature is high
    enough to excite the electrons within an atom.
   Ultraviolet frequencies can be produced from the discharge of an
    electric arc.
   X-rays are produced by the sudden deceleration of high-speed
    electrons.
   And, finally, gamma rays are radiation from nuclear decay.
                        VISIBLE LIGHT
   Our eyes are only sensitive to visible light.
   Only waves with frequencies between about 4.0 x 1014 Hz
    and 7.9 x 1014 Hz are perceived by the human eye as visible
    light (visible light is the most narrow in the spectrum)
   Usually visible light is discussed in terms of wavelengths (in
    vacuum) rather than frequencies.
   The wavelengths of visible light are extremely small and,
    therefore, are normally expressed in nanometers (nm);
         1 nm = 10-9 m.
   An obsolete (non-SI) unit occasionally used for wavelengths
    is the angstrom (Å);
         1 Å = 10-10 m.
Example 1: The Wavelength of Visible Light
Find the range in wavelengths (in vacuum) for visible light in the
frequency range between 4.0 x 1014 Hz (red light) and 7.9 x 1014 Hz
(violet light). Express the answers in nanometers.
                      VISIBLE LIGHT
   The eye/brain recognizes light of different wavelengths as
    different colors. A wavelength of 750 nm (in vacuum) is
    approximately the longest wavelength of red light, whereas
    380 nm (in vacuum) is approximately the shortest
    wavelength of violet light. Between these limits are found
    the other familiar colors.
   The association between color and wavelength in the visible
    part of the electromagnetic spectrum is well known.
   The wavelength also plays a central role in governing the
    behavior and use of electromagnetic waves in all regions of
    the spectrum. For instance, the next Conceptual Example
    considers the influence of the wavelength on diffraction. 
Conceptual Example 2: The Diffraction of AM and FM Radio Waves
As discussed in previous section, diffraction is the ability of
a wave to bend around an obstacle or around the edges of an
opening. Based on that discussion, which type of radio wave
would you expect to bend more readily around an obstacle
such as a building, (a) an AM radio wave or (b) an FM radio wave?
Section 10:
The Doppler Effect
THE DOPPLER EFFECT
    Have you ever heard an approaching fire truck and noticed
     the change in the sound of the siren as the truck passes?
       While the fire truck approaches, the pitch of the siren
        is relatively high, but as it passes and moves away,
        the pitch suddenly drops.
    • Something similar, but less familiar, occurs when an
      observer moves towards or away from a stationary source
      of sound.
    • Such phenomena are collectively referred to as the Doppler
      Effect.
THE DOPPLER EFFECT
   The Doppler effect is the apparent change in the frequency
    of a wave motion when there is relative motion between the
    source and the observer.
   Named after Christian Johann Doppler (1803-1853)
   Doppler effect occurs in both sound waves (siren or train
    horn) and light waves
   Amount of the shift and its sign depends on
     – relative speed of the source & observer
     – direction (towards or away)
Moving Source
• Consider the sound emitted by a siren
  of a stationary fire truck
• Each solid blue arc represents a
  condensation of the sound wave
• In Figure (a). sound pattern is
  symmetrical, listener standing in
  front of or behind the truck detect
  the same number of condensations
  per second, and consequently, hear
  same frequency.
• Once truck begins to move ahead of
  truck the condensations are now closer
  together, resulting in decrease in
  wavelength of the sound (Figure b.)
• This “bunching-up” is because truck
  “gains ground” on a previously emitted
  condensation before emitting the next
  one.
Moving Source 2..
• Since the condensations are closer
  together, the observer standing in front
  of the truck senses more of them
  arriving per second than she does when
  the truck is stationary.
• The increased rate of arrival
  corresponds to a greater sound
  frequency, which the observer hears as a
  higher pitch.
• Behind the moving truck, the
  condensations are farther apart than
  they are when the truck is stationary.
• This increase in the wavelength occurs
  because the truck pulls away from
  condensations emitted toward the rear.
• Consequently, fewer condensations per
  second arrive at the ear of an observer
  behind the truck, corresponding to a
  smaller sound frequency or lower pitch. 
Moving Source 3..
• If the stationary siren in Figure a.
  emits a condensation at the time t =0
  s, it will
  emit the next one at time T, where T is
  the period of the wave.
• The distance between these two
  condensations is the wavelength (λ) of
  the sound produced by the stationary
  source
Moving Source 4..
Moving Source 5..
• But for the stationary siren, we have        and
                                                     Source moving
                                                     toward stationary
                                                     observer:
                                          ….Eqn 1.
Moving Source - Away
• The same reasoning that led to Equation 1 can be used to
  obtain an expression for the observed frequency fo:
                                                Source moving
                                                away from
                                                stationary
                                     ….Eqn 2.
                                                observer
Example 1: The Sound of a Passing Train
A high-speed train is traveling at a speed of 44.7 m/s (100 mi/h) when
the engineer sounds the 415 Hz warning horn. The speed of sound is 343
m/s. What are the frequency and wavelength of the sound, as perceived
by a person standing at a crossing, when the train is (a) approaching and
(b) leaving the crossing?
Moving Observer
Moving Observer 2..
                                 Observer moving
                                 toward stationary
                      ….Eqn 3.   source:
Moving Observer - Away
                             Observer moving
                             away from
                             stationary source:
                  ….Eqn 4.
Moving Source vs Moving Observer
• It should be noted that the physical mechanism producing
  the Doppler effect is different when the source moves and
  the observer is stationary than when the observer moves
  and the source is stationary:
Example 2: An Accelerating Speedboat and the Doppler Effect
A speedboat, starting from rest, moves along a straight line away from a
dock. The boat has a constant acceleration of +3.00 m/s2 (see figure below).
Attached to the dock is a siren that is producing a 755 Hz tone. If the air
temperature is 20 °C, what is the frequency of the sound heard by a person
on the boat when the boat’s displacement from the dock is +45.0 m?
An Accelerating Speedboat
Moving Source vs Moving Observer
summary
   Moving Source
       change in   f
   Moving Observer
      change in relative velocity  f
   Moving Source and Observer
      change in  and relative velocity  f
General Case
                                               Source and
                                               observer both
                                               moving:
                                    ….Eqn 5.
• In the numerator, the plus sign applies when the observer moves toward the
  source, and the minus sign applies when the observer moves away from
  source.
• In the denominator, the minus sign is used when the source moves toward
  the observer, and the plus sign is used when the source moves away from
  the observer.
    Equations –
    Moving Source and Moving Observer
    vs         vo            vs             vo
S          O                       S   O
    vs      vo                vs           vo
S                   O              S             O
 source vs    observer vo observed
                          frequency
                              fo
stationary    stationary    = fs
stationary    receding      < fs
stationary    approachin    > fs
              g
receding      stationary    < fs
approaching   stationary    > fs
receding      receding      < fs
approaching   approachin    > fs
              g
approaching   receding       ?
receding      approachin     ?
              g                       CP 595
THE DOPPLER EFFECT IN LIGHT
   Works same as it does for sound
      Light moving away from the observer
         o Decrease in measured frequency
         o Wavelength gets longer: REDSHIFT
       Light moving towards the observer
          o Increase in measured frequency
          o Wavelength gets shorter: BLUESHIFT
Red Shift
   A r e d s h i f t i s an y d e c r e as e i n f r e q u e n c y , w i t h a
    corresponding increase in wavelength, of an electromagnetic
    wave;
   In visible light, this shifts the color from the blue end of the
    spectrum to the red end.
   The Doppler Red shift results from the relative motion of
    the light emitting object and the observer. If the source of
    light is moving away from you then the wavelength of the
    light is stretched out, i.e., the light is shifted towards the
    red.
Blue Shift
   A bl u e s h i f t i s an y i n c re as e i n f re q u e n c y , w i th a
    co rresp o nding decrease in w avelength, o f an
    electromagnetic wave;
   In visible light, this shifts the color from the red end of
    the spectrum to the blue end.
   The Doppler Blue shift results from the relative motion of
    the light emitting object and the observer. If the source of
    light is moving toward you then the wavelength of the light
    is compressed, i.e., the light is shifted towards the blue.
Light experiences the Doppler Effect too!
             Objects that
             are moving
             quickly away
             from us have
             their
             wavelength
             shifted
             toward the
             RED end of
             the
                               Objects that are moving
             spectrum
                               quickly toward us have their
                               wavelength shifted toward
                               the BLUE end of the
                               spectrum
USES OF THE DOPPLER SHIFT:
In Astronomy
   Radio astronomers can find the motion of a source (stars,
    galaxies, gases, etc.) by observing whether the emission or
    absorption lines in its spectrum are shifted in wavelength
    relative to their wavelengths at rest
Light From Distant Cosmic Objects is Doppler
Shifted
                              The same spectral lines
                              seen in a distant galaxy
Sun’s optical                 cluster - shifted to a
spectral lines                longer wavelength / lower
                              frequency by the Doppler
                              Effect
        Radar and the Doppler Effect in Meteorology
           Radar waves are scattered off of a target in the atmosphere
            such as rain drops, which act as tracers for the wind’s velocity.
           So…if the wind is moving towards the radar, the returning radio
            waves will be shifted to higher frequencies, and if moving away
            from the radar, the radio waves will be shifted to lower
            frequencies.
                                       higher
lower
NEXRAD = NEXt Generation Weather RADar
(based on Doppler-shifted radar) is used to
identify storms that are likely to spawn
                                                Doppler Radar for Hurricane Katrina
tornadoes
The Doppler Effect in Meteorology
   Radar (Radio Detection and Ranging)
    transmits microwaves to detect
    precipitation particles in the atmosphere
    (such as rain, snow, and hail).
   After a radar sends out a signal, it "
    listens" for returning signals. A returning
    signal, called an echo, occurs when the
    transmitted signal strikes and reflects
    off objects (raindrops, ice, snow, trees,
    buildings, mountains, birds, or even
    insects) within its path.                     A Doppler Radar Tower
   Part of the reflected signal is received
    back at the radar. The amount and type
    of precipitation that is falling can be
    determined.
 The Doppler Effect in Bats
 Bats navigate by emitting high frequency sound
     waves
 (ultrasonic) and then detecting the reflected
     waves…
 An example: Imagine the bat and the moth flying
     towards each other. The moth will “receive”
     a frequency that is higher than the bat’s
     emitted frequency.
When the sound reflects off the moth,
the moth now acts as a “new source” and the bat
is the receiver  a 2nd doppler shift!!
The frequency of this “new source” for the 2nd doppler shift will be the
frequency received or heard by the moth from the 1st doppler shift.
The frequency received by the bat will be even higher than the frequency the
moth “heard.”
The bat’s brain then “calculates” the speed and direction of the moth’s
motion from the difference in the emitted and received frequencies… lunch!
The Doppler Effect in Dolphins
•   Dolphins hunt underwater by
    emitting ultrasonic sounds and
    detecting the reflections.
Radar Guns
• All waves (not just sound) can be doppler shifted. A police
  radar gun bounces a high frequency radio wave off of a
  moving car. The system then calculates the speed of the
  car by comparing the frequency of the emitted “radar”
  waves with the frequency of the reflected waves.
• … just like the bat, there are 2 doppler shifts.
Reading Assignment
   Define the following with appropriate diagrams:
   Sonic boom
   Shock waves
References
   Cutnell J.D. & Johnson K.W. (2010) Introduction to Physics,
    8th Ed. John Wiley & Sons Pvt Ltd
 END OF “DOPPLER EFFECT”
END OF PHY222 CLASS SLIDES