Electromagnetic Wave Propagation - PowerPoint PPT Presentation

1 / 12
About This Presentation
Title:

Electromagnetic Wave Propagation

Description:

We will start our discussion by considering fields in the time domain. ... Poynting vector using the E(z,t) and H(z,t) can be determined through ... – PowerPoint PPT presentation

Number of Views:76
Avg rating:3.0/5.0
Slides: 13
Provided by: kuk8
Category:

less

Transcript and Presenter's Notes

Title: Electromagnetic Wave Propagation


1
CHAPTER 4
ELECTROMAGNETIC FIELDS THEORY
  • Electromagnetic Wave Propagation

2
Power and Poynting Vector
  • The dimension of E and H are V/m and A/m
    respectively. Hence, the vector ExH has VA/m2 as
    dimension, which is power density W/m2.
  • The cross product ExH results in a vector along
    the direction of propagation that is the
    direction of the energy flow.
  • The vector ExH is known as the power density or
    Poynting vector.
  • Poynting vector P E x H
  • which is directed along the direction of the
  • electromagnetic energy flow

3
Power and Poynting Vector
  • Poynting Theorem states that
  • The net power flowing out of a given volume v is
    equal to the time rate of decrease in the energy
    stored between v minus the conduction losses

4
Power and Poynting Vector
  • We will start our discussion by considering
    fields in the time domain.
  • From Maxwells equation for a time-varying field,
  • If we take the dot product of both sides of
    Maxwells curl of H equation with E, we obtain

5
Power and Poynting Vector
  • Rearranging eq (2), we have
  • Also, from Maxwells curl of E equation, we have
  • Substituting this into the former eq (3), we
    obtain

6
Power and Poynting Vector
  • If the medium is simple, we can also write
  • Substituting (5) and (6) into this into (4) we
    obtain

7
Power and Poynting Vector
  • Integrating eq (7) over an arbitrary volume v, we
    get
  • Finally, we can use the divergence theorem to
    express the left-hand side as a surface integral
    over the surface S that bounds v

8
Power and Poynting Vector
  • The ohmic power dissipated inside v
  • The rate of decrease in energy stored in electric
    and magnetic fields

9
Power and Poynting Vector
  • Poynting vector using the E(z,t) and H(z,t) can
    be determined through
  • P (z,t) E(z,t) x H(z,t) (9)
  • Time-average poynting vector can determined by
    integrating eq (9) over the period T,

10
Power and Poynting Vector
  • Total time-average power crossing a given surface
    is given by

11
Example 1
  • In a free space medium,
  • Find
  • (a) H field
  • (b) The time-average power carried by the wave
  • (c) The total power crossing of
    plane

12
Exercise 1
  • In a free space medium,
  • Find the total power passing through
  • (a) A square plate of side 10 cm on plane
  • (b) A circular disk of radius 5 cm on plane
Write a Comment
User Comments (0)
About PowerShow.com