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Electromagnetic
Wave Propagation
IRFAN SULTAN
INSTRUCTOR (TELECOM.)
GOVT. COLLEGE OF TECHNOLOGY
Contents
 Introduction to EM Waves.
 Electromagnetic Spectrum
 Wave Propagation in Lossy Dielectrics
 Plane Waves in Free Space
 Plane Waves in Good Conductors
Introduction to EM-Waves
 Electromagnetic Waves, also abbreviated as EM-Waves, are the waves
which consist of both Electric and Magnetic Fields and travel at a speed
same as that of light, i.e. 3x108 m/sec
 All forms of electromagnetic radiation consist of perpendicular oscillating
electric and magnetic fields.
Properties of EM-Waves
 Invisible
 Travel at speed of light
 Consist of Electric and Magnetic fields
 Electric Field, Magnetic Field and Direction of Propagation of an EM wave
are all perpendicular to each other
 Their Electric and Magnetic fields cannot be separated from each other
 The total energy of an EM wave is equally divided between Electric and
Magnetic fields
 When they pass through a metallic conductor they produce voltage across
the conductor
Properties of EM-Waves
 They don’t need any medium to travel
 Their intensity is same all around in free space
 When they travel from one place to another their power (intensity) is
reduced, i.e. they suffer from attenuation
 When they enter from one medium to another:
 Their form of energy changes, i.e. they suffer from Absorption
 They are diverted from their path, this process is called refraction
 When they pass through a hole they bent along sides when leaving the
hole, this process is called Deflection
Refraction, Absorption and Diffraction
Refraction
Reflection Diffraction
Absorption
Electromagnetic Spectrum
 EM Spectrum is the range of wavelengths or frequencies over which
electromagnetic radiation extends.
 It consists of different frequency bands which are basically groups of
certain frequency ranges.
Electromagnetic Spectrum
Waves
Longitudinal Waves Transverse Waves
Electromagnetic Waves
Electromagnetic Spectrum
Radiowave
Microwave
Infra-Red
Light
Ultra-Violet
X-ray
Gamma ray
Applications
Sound waves
Classified into
Comprises of
Some tips to help you to remember:
 EM Spectrum
Raja’s Mother Is Visiting Uncle Xavier’s Garden
 Visible Light Spectrum
Run Off You Girls Boys In View
Radio
wave
Micro
wave
Infra-red
Rays
Visible
light
Ultra-violet
ray
X-rays Gamma
rays
red orange yellow green blue indigo violet
Wave Propagation in Lossy Dielectrics
 A Lossy Dielectric is basically a medium which reduce the power of EM
waves, due to its “Poor Condition”, when they travel through it.
 In other words, a Lossy Dielectric is a practical conducting medium that is
neither a good conductor nor a good insulator.
 The following terms are used to describe the losses in a propagating wave:
 Attenuation Coefficient 𝛼
 Phase Coefficient 𝛽
 Attenuation Coefficient is measured in Neper Per Meter (Np/m) or Decibel
Per Meter (dB/m)
 1Np = 20log(e) = 8.686 dB
 Formulas for Velocity and Wavelength of a wave are:
Wave Propagation in Lossy Dielectrics
 Formulas for Attenuation and Phase coefficients are:
𝜎 = sigma = Conductivity
𝜇 = mu = Permeability
𝜔 = omega = Angular velocity
ε = epsilon = Permittivity
Plane Waves in Free Space
 This is a special case for which:
 Permeability 𝜇 = 𝜇𝑜 (Permeability of free space) = µ0 = 4π × 10−7 H
 Conductivity 𝜎 = 0
 Permittivity ε = εo (Permittivity of free space) = 8.85 x 10-12 F/m

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EM Wave Propagation

  • 1. Electromagnetic Wave Propagation IRFAN SULTAN INSTRUCTOR (TELECOM.) GOVT. COLLEGE OF TECHNOLOGY
  • 2. Contents  Introduction to EM Waves.  Electromagnetic Spectrum  Wave Propagation in Lossy Dielectrics  Plane Waves in Free Space  Plane Waves in Good Conductors
  • 3. Introduction to EM-Waves  Electromagnetic Waves, also abbreviated as EM-Waves, are the waves which consist of both Electric and Magnetic Fields and travel at a speed same as that of light, i.e. 3x108 m/sec  All forms of electromagnetic radiation consist of perpendicular oscillating electric and magnetic fields.
  • 4. Properties of EM-Waves  Invisible  Travel at speed of light  Consist of Electric and Magnetic fields  Electric Field, Magnetic Field and Direction of Propagation of an EM wave are all perpendicular to each other  Their Electric and Magnetic fields cannot be separated from each other  The total energy of an EM wave is equally divided between Electric and Magnetic fields  When they pass through a metallic conductor they produce voltage across the conductor
  • 5. Properties of EM-Waves  They don’t need any medium to travel  Their intensity is same all around in free space  When they travel from one place to another their power (intensity) is reduced, i.e. they suffer from attenuation  When they enter from one medium to another:  Their form of energy changes, i.e. they suffer from Absorption  They are diverted from their path, this process is called refraction  When they pass through a hole they bent along sides when leaving the hole, this process is called Deflection
  • 6. Refraction, Absorption and Diffraction Refraction Reflection Diffraction Absorption
  • 7. Electromagnetic Spectrum  EM Spectrum is the range of wavelengths or frequencies over which electromagnetic radiation extends.  It consists of different frequency bands which are basically groups of certain frequency ranges.
  • 9. Waves Longitudinal Waves Transverse Waves Electromagnetic Waves Electromagnetic Spectrum Radiowave Microwave Infra-Red Light Ultra-Violet X-ray Gamma ray Applications Sound waves Classified into Comprises of
  • 10. Some tips to help you to remember:  EM Spectrum Raja’s Mother Is Visiting Uncle Xavier’s Garden  Visible Light Spectrum Run Off You Girls Boys In View Radio wave Micro wave Infra-red Rays Visible light Ultra-violet ray X-rays Gamma rays red orange yellow green blue indigo violet
  • 11. Wave Propagation in Lossy Dielectrics  A Lossy Dielectric is basically a medium which reduce the power of EM waves, due to its “Poor Condition”, when they travel through it.  In other words, a Lossy Dielectric is a practical conducting medium that is neither a good conductor nor a good insulator.  The following terms are used to describe the losses in a propagating wave:  Attenuation Coefficient 𝛼  Phase Coefficient 𝛽
  • 12.  Attenuation Coefficient is measured in Neper Per Meter (Np/m) or Decibel Per Meter (dB/m)  1Np = 20log(e) = 8.686 dB  Formulas for Velocity and Wavelength of a wave are: Wave Propagation in Lossy Dielectrics  Formulas for Attenuation and Phase coefficients are: 𝜎 = sigma = Conductivity 𝜇 = mu = Permeability 𝜔 = omega = Angular velocity ε = epsilon = Permittivity
  • 13. Plane Waves in Free Space  This is a special case for which:  Permeability 𝜇 = 𝜇𝑜 (Permeability of free space) = µ0 = 4π × 10−7 H  Conductivity 𝜎 = 0  Permittivity ε = εo (Permittivity of free space) = 8.85 x 10-12 F/m

Editor's Notes

  • #14: The permeability constant (µ0), also known as the magnetic constant or the permeability of free space, is a measure of the amount of resistance encountered when forming a magnetic field in a classical vacuum. The magnetic constant has the exact (defined) value (µ0 = 4π × 10−7 H. Permittivity: the ability of a substance to store electrical energy in an electric field.
  • #15: Skin depth is a measure of how far electrical conduction takes place in a conductor, and is a function of frequency. At DC (0 Hz) the entire conductor is used, no matter how thick it is. The skin depth is a measure of the penetration of a plane electromagnetic wave into a material.