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WAVE PROPAGATION
Areeba Shujaat
(2012-TE-16)
TYPES OF WAVES
Vibration is in the same direction as wave pulse (parallel to wave pulse)
Vibration is at 900 (right angles) to wave pulse
DEFINITION OF E.M.WAVES
The wave of the electric field and the wave of the magnetic field are
propagated perpendicularly to the direction of propagation and to
each other.
• They are Transverse waves without a medium. (They can travel
through empty space)
• They travel as vibrations in electrical and magnetic fields
EM waves in free
space
• v2 = 1/(oµo) so v = 3 x 108 m/s
– o = 8.855 x 10-12 Farads/m
– µo = 1.2566 x 10-6 Henrys/m
• EM waves in free space propagate
freely without attenuation
• What is a plane wave?
– Example is a wave propagating
along the x-direction
– Fields are constant in y and z
directions, but vary with time
and space along the x-
direction
– Most propagating radio (EM)
waves can be thought of a
plane waves on the scale of
the receiving antenna
Real-life application: Antenna
RADIO FREQUENCY
INTERFACE
Radio-frequency
interference occurs when
the signal emitted by one
device gets unintentionally
picked up by another—
creating audible noise or a
compromised connection.
Some interference is due
to badly shielded wires or
components, but some is
just the result of too many
gadgets crowded into a
limited spectrum.
Electro-magnetic Interference
• Electromagnetic interference, that is: the
influence of strong magnetic or electric fields
on avr microcontrollers results in random
failures.
• What to do about EMI? Shielding
Polarization
• Defined as the orientation of the electric field
(E-plane) of an electromagnetic wave
• Vertically Polarized Antenna
– Electric field is perpendicular to the Earth’s surface
– e.g., Broadcast tower for AM radio, “whip” antenna on an automobile
• Horizontally Polarized Antenna
– Electric field is parallel to the Earth’s surface
– e.g., Television transmission (U.S.)
• Circular Polarized Antenna
– Wave radiates energy in both the horizontal and vertical planes and all
planes in between
Wave fronts
• A wave front is a plane joining all points of
equal phase in a wave
• Take a point in space. Imagine waves radiating
outward in all directions from this point. The
result would resemble a sphere. The point of
radiation is called the isotropic point source
Normalized
Antenna Pattern
In free space:
 = 1.26 x 10-6 H/m
 = 8.85 x 10-12 F/m
 = 377 
Common Characteristics of E.M.Waves
• Reflection
• Refraction
Diffraction
Based on Huygen’s principle (1690)
Each point on a wavefront can be thought of as an isotropic
point or a source of secondary spherical energy
Waves traveling in straight lines bend around obstacles
Scattering
• The change in direction of a
particle or photon because of a
collision with another particle or
a system.
Ground Waves
• A radio wave can leave the antenna in a straight line and
progress along the ground. ground waves leave an antenna in
all directions in the case of a vertical one and mainly from their
broadside in the case of a horizontal antenna. Ground waves
are always vertically polarized, because a horizontally polarized
ground wave would be shorted out by the conductivity of the
ground. Because ground waves are actually in contact with the
ground, they are greatly affected by the ground’s properties.
Because ground waves are actually in contact with the ground,
they are greatly affected by the ground’s properties. Because
ground is not a perfect electrical conductor, ground waves are
attenuated as they follow the earth’s surface. This effect is
more pronounced at higher frequencies, limiting the
usefulness of ground wave propagation to frequencies below 2
MHz. Ground waves will propagate long distances over sea
water, due to its high conductivity
SPACE WAVE PROPAGATION
• The EM wave that
propagates from the
transmitter to the receiver
in the earth’s troposphere is
called “Space Wave”.
• Troposphere is the region
of the atmosphere with in
15km above the surface of
the earth.
• The Maximun line of sight
distance between two
antenns depends on the
height of each antenna.
Sky Wave
• Radio waves radiated from the transmitting antenna
in a direction toward the ionosphere
• Long distance transmissions
• Sky wave strike the ionosphere, is refracted back to
ground, strike the ground, reflected back toward the
ionosphere, etc until it reaches the receiving
antenna
• Skipping is he refraction and reflection of sky waves
Atmospheric Phenomenon
• Three layers:
– Troposphere: earth’s surface to about 6.5 mi
– Stratosphere: extends from the troposphere upwards
for about 23 mi
– Ionosphere: extends from the stratosphere upwards
for about 250mi
– Beyond this layer is free space
• Temperature in the stratosphere is believed to be fairly
constant and is not subject to temperature changes or
inversions and will not cause significant refractions
• This is called an isothermal region
• The ionic density in the ionosphere varies from very
dense at the border between the ionosphere and
stratosphere to very low density as it approaches free
space
• The ions in the far reaches of the ionosphere are easily
susceptible to the sun’s radiation with the susceptibility
reducing as one approaches the stratosphere
• Three layers
– D: low frequencies can
be refracted but the high
frequencies tend to pass
on through
– E: signals as high as
20MHz can be refracted
while higher ones pass
through
– F: during the day light
hours there are two
layers:
• F1 and F2
Solar Cycle
• Every 11 years the sun undergoes a period
of activity called the "solar maximum",
followed by a period of quiet called the
"solar minimum". During the solar maximum
there are many sunspots, solar flares, and
coronal mass ejections, all of which can
affect communications and weather here on
Earth.
• The Sun goes through a periodic rise and fall in
activity which affects HF communications; solar
cycles vary in length from 9 to 14 years. At solar
minimum, only the lower frequencies of the HF
band will be supported by the ionosphere, while at
solar maximum the higher frequencies will
successfully propagate, figure 1.4. This is because
there is more radiation being emitted from the Sun
at solar maximum, producing more electrons in the
ionosphere which allows the use of higher
frequencies.
How Do Sunspots Affect Earth
• The Earth is affected by
both solar flares and
sunspots. Solar flares emit
high-speed particles which
cause auroras, known in the
northern hemisphere as
Northern Lights. The image
shown here is a real-time
satellite image of the Earth's
auroral region above the
North Pole. From the
ground auroras appear as
shimmering curtains of red
and green light in the sky.
• Particles from solar flares can also disrupt
radio communication, and the radiation
from the flares can give passengers in
airplanes a dose of radiation equivalent to
a medical X-ray. Sunspots may have a
long-term connection with the Earth's
climate. Scientists are currently debating
whether ice ages on Earth are related to
the Sun having fewer sunspots than usual.
How Does HF Radio Work Over
Long Distances?
• An HF signal transmitted from the earth may travel some
way through the ionosphere before being "bent" back down
towards the ground. This occurs due to the interaction
between the HF signal and electrically charged particles in
the ionosphere. The signal can then "bounce" off the ground
back into the ionosphere, return to the earth again, and so
on. The distance a given HF signal will travel depends on the
frequency, transmitter power, take-off angle relative to the
ground and the state of the ionosphere through which it is
travelling.
How Do Conditions Affecting the Use
of HF Radio Vary Over Time?
• Extreme Ultraviolet (EUV) radiation from the sun
creates the ionosphere. The EUV radiation arises from
the bright and hot regions which overlie sunspots
(areas of strong magnetic fields on the sun's surface).
As the sun progresses through its eleven year cycle of
activity, the number and size of sunspots will vary, as
will the level of EUV radiation. Changes to the
ionosphere that result from this mean that conditions
affecting the use of HF radio will also change over the
solar cycle.
What Kind of Disturbances Can
Degrade HF Communications?
• Short-Wave Fadeouts
• Short-Wave Fadeouts -
short lived (up to two
hours) disturbances, in
which solar flare activity
results in the absorption
of lower frequency HF
signals. These will only
affect signals passing
through the daylight
ionosphere
Ionospheric Storms
• Ionospheric Storms - large
scale changes in the
chemical composition of
the ionosphere resulting
in changes to the MUF.
Decreased MUFs restrict
the frequencies available
for use over a given
distance. Ionospheric
storms normally last for
one to two days.
Critical Frequency
• The highest frequency that will be returned
to the earth when transmitted vertically
under given ionospheric conditions
Critical Angle
• The highest angle with respect to a vertical line at
which a radio wave of a specified frequency can be
propagated and still be returned to the earth from
the ionosphere
Maximum usable frequency (MUF)
• The highest frequency that is returned to the earth from
the ionosphere between two specific points on earth
Optimum Working frequency
• The frequency that provides for the most consistent
communication path via sky waves
wave propagationn

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wave propagationn

  • 2. TYPES OF WAVES Vibration is in the same direction as wave pulse (parallel to wave pulse) Vibration is at 900 (right angles) to wave pulse
  • 3. DEFINITION OF E.M.WAVES The wave of the electric field and the wave of the magnetic field are propagated perpendicularly to the direction of propagation and to each other. • They are Transverse waves without a medium. (They can travel through empty space) • They travel as vibrations in electrical and magnetic fields
  • 4. EM waves in free space • v2 = 1/(oµo) so v = 3 x 108 m/s – o = 8.855 x 10-12 Farads/m – µo = 1.2566 x 10-6 Henrys/m • EM waves in free space propagate freely without attenuation • What is a plane wave? – Example is a wave propagating along the x-direction – Fields are constant in y and z directions, but vary with time and space along the x- direction – Most propagating radio (EM) waves can be thought of a plane waves on the scale of the receiving antenna
  • 6. RADIO FREQUENCY INTERFACE Radio-frequency interference occurs when the signal emitted by one device gets unintentionally picked up by another— creating audible noise or a compromised connection. Some interference is due to badly shielded wires or components, but some is just the result of too many gadgets crowded into a limited spectrum.
  • 7. Electro-magnetic Interference • Electromagnetic interference, that is: the influence of strong magnetic or electric fields on avr microcontrollers results in random failures. • What to do about EMI? Shielding
  • 8. Polarization • Defined as the orientation of the electric field (E-plane) of an electromagnetic wave
  • 9. • Vertically Polarized Antenna – Electric field is perpendicular to the Earth’s surface – e.g., Broadcast tower for AM radio, “whip” antenna on an automobile • Horizontally Polarized Antenna – Electric field is parallel to the Earth’s surface – e.g., Television transmission (U.S.) • Circular Polarized Antenna – Wave radiates energy in both the horizontal and vertical planes and all planes in between
  • 10. Wave fronts • A wave front is a plane joining all points of equal phase in a wave • Take a point in space. Imagine waves radiating outward in all directions from this point. The result would resemble a sphere. The point of radiation is called the isotropic point source
  • 11. Normalized Antenna Pattern In free space:  = 1.26 x 10-6 H/m  = 8.85 x 10-12 F/m  = 377 
  • 12. Common Characteristics of E.M.Waves • Reflection
  • 14. Diffraction Based on Huygen’s principle (1690) Each point on a wavefront can be thought of as an isotropic point or a source of secondary spherical energy Waves traveling in straight lines bend around obstacles
  • 15. Scattering • The change in direction of a particle or photon because of a collision with another particle or a system.
  • 16. Ground Waves • A radio wave can leave the antenna in a straight line and progress along the ground. ground waves leave an antenna in all directions in the case of a vertical one and mainly from their broadside in the case of a horizontal antenna. Ground waves are always vertically polarized, because a horizontally polarized ground wave would be shorted out by the conductivity of the ground. Because ground waves are actually in contact with the ground, they are greatly affected by the ground’s properties. Because ground waves are actually in contact with the ground, they are greatly affected by the ground’s properties. Because ground is not a perfect electrical conductor, ground waves are attenuated as they follow the earth’s surface. This effect is more pronounced at higher frequencies, limiting the usefulness of ground wave propagation to frequencies below 2 MHz. Ground waves will propagate long distances over sea water, due to its high conductivity
  • 17.
  • 18. SPACE WAVE PROPAGATION • The EM wave that propagates from the transmitter to the receiver in the earth’s troposphere is called “Space Wave”. • Troposphere is the region of the atmosphere with in 15km above the surface of the earth. • The Maximun line of sight distance between two antenns depends on the height of each antenna.
  • 20. • Radio waves radiated from the transmitting antenna in a direction toward the ionosphere • Long distance transmissions • Sky wave strike the ionosphere, is refracted back to ground, strike the ground, reflected back toward the ionosphere, etc until it reaches the receiving antenna • Skipping is he refraction and reflection of sky waves
  • 21. Atmospheric Phenomenon • Three layers: – Troposphere: earth’s surface to about 6.5 mi – Stratosphere: extends from the troposphere upwards for about 23 mi – Ionosphere: extends from the stratosphere upwards for about 250mi – Beyond this layer is free space
  • 22.
  • 23. • Temperature in the stratosphere is believed to be fairly constant and is not subject to temperature changes or inversions and will not cause significant refractions • This is called an isothermal region • The ionic density in the ionosphere varies from very dense at the border between the ionosphere and stratosphere to very low density as it approaches free space • The ions in the far reaches of the ionosphere are easily susceptible to the sun’s radiation with the susceptibility reducing as one approaches the stratosphere
  • 24. • Three layers – D: low frequencies can be refracted but the high frequencies tend to pass on through – E: signals as high as 20MHz can be refracted while higher ones pass through – F: during the day light hours there are two layers: • F1 and F2
  • 25. Solar Cycle • Every 11 years the sun undergoes a period of activity called the "solar maximum", followed by a period of quiet called the "solar minimum". During the solar maximum there are many sunspots, solar flares, and coronal mass ejections, all of which can affect communications and weather here on Earth.
  • 26.
  • 27. • The Sun goes through a periodic rise and fall in activity which affects HF communications; solar cycles vary in length from 9 to 14 years. At solar minimum, only the lower frequencies of the HF band will be supported by the ionosphere, while at solar maximum the higher frequencies will successfully propagate, figure 1.4. This is because there is more radiation being emitted from the Sun at solar maximum, producing more electrons in the ionosphere which allows the use of higher frequencies.
  • 28. How Do Sunspots Affect Earth • The Earth is affected by both solar flares and sunspots. Solar flares emit high-speed particles which cause auroras, known in the northern hemisphere as Northern Lights. The image shown here is a real-time satellite image of the Earth's auroral region above the North Pole. From the ground auroras appear as shimmering curtains of red and green light in the sky.
  • 29. • Particles from solar flares can also disrupt radio communication, and the radiation from the flares can give passengers in airplanes a dose of radiation equivalent to a medical X-ray. Sunspots may have a long-term connection with the Earth's climate. Scientists are currently debating whether ice ages on Earth are related to the Sun having fewer sunspots than usual.
  • 30.
  • 31. How Does HF Radio Work Over Long Distances? • An HF signal transmitted from the earth may travel some way through the ionosphere before being "bent" back down towards the ground. This occurs due to the interaction between the HF signal and electrically charged particles in the ionosphere. The signal can then "bounce" off the ground back into the ionosphere, return to the earth again, and so on. The distance a given HF signal will travel depends on the frequency, transmitter power, take-off angle relative to the ground and the state of the ionosphere through which it is travelling.
  • 32. How Do Conditions Affecting the Use of HF Radio Vary Over Time?
  • 33. • Extreme Ultraviolet (EUV) radiation from the sun creates the ionosphere. The EUV radiation arises from the bright and hot regions which overlie sunspots (areas of strong magnetic fields on the sun's surface). As the sun progresses through its eleven year cycle of activity, the number and size of sunspots will vary, as will the level of EUV radiation. Changes to the ionosphere that result from this mean that conditions affecting the use of HF radio will also change over the solar cycle.
  • 34. What Kind of Disturbances Can Degrade HF Communications? • Short-Wave Fadeouts • Short-Wave Fadeouts - short lived (up to two hours) disturbances, in which solar flare activity results in the absorption of lower frequency HF signals. These will only affect signals passing through the daylight ionosphere
  • 35. Ionospheric Storms • Ionospheric Storms - large scale changes in the chemical composition of the ionosphere resulting in changes to the MUF. Decreased MUFs restrict the frequencies available for use over a given distance. Ionospheric storms normally last for one to two days.
  • 36. Critical Frequency • The highest frequency that will be returned to the earth when transmitted vertically under given ionospheric conditions
  • 37. Critical Angle • The highest angle with respect to a vertical line at which a radio wave of a specified frequency can be propagated and still be returned to the earth from the ionosphere
  • 38. Maximum usable frequency (MUF) • The highest frequency that is returned to the earth from the ionosphere between two specific points on earth
  • 39. Optimum Working frequency • The frequency that provides for the most consistent communication path via sky waves