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Poynting vector:
Poynting Vector ‘S’ is defined as the cross product
of the vectors E & H.
The direction of power flow at any point is
normal to both E & H vectors.
The Unit is watts/m2
                 S=ExH
Poynting Theorem from Maxwell’s Equations:
Maxwell’s equation in the point form is

Equation (1)
Taking dot product with ‘E’ on both sides




From vector identity,



Equation (2)
Substituting equation (2) in (1)
 Equation (3) is




From Maxwell’s Equation
Equation (4)



Substituting
 in Equation (4)
Integrating throughout the volume




Total Power    Power         Rate of energy stored
               dissipation

Using divergence theorem
Power flow in a co-axial cable

 Consider a co-axial cable which has a dc
voltage ‘V’ between the conductors and a
steady current I flowing in the inner and outer
conductors.
      The radius of inner and outer conductor
are ‘a’ and ‘b’ respectively.


         +                       b
                                     a
                   I
     V                                   Resistance

         -
By ampere’s Law:




            Circumference of circular path
            between a and b =2πr
E due to an infinitely long conductor


                            Equation (1)

Where λ is the charge density.
     The potential difference between the
conductors is


                             Equation (2)


 E in terms of V from (1) and (2) is
Power density

Since E and H are always perpendicular to
each other
The total power will be given by the
integration of power density P over any cross
section surface.

 Let the elemental surface already be 2πrdr


Total power
i.e. The power flow along the cable is the
product of V and I

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Poynting vector

  • 1. Poynting vector: Poynting Vector ‘S’ is defined as the cross product of the vectors E & H. The direction of power flow at any point is normal to both E & H vectors. The Unit is watts/m2 S=ExH Poynting Theorem from Maxwell’s Equations: Maxwell’s equation in the point form is Equation (1)
  • 2. Taking dot product with ‘E’ on both sides From vector identity, Equation (2)
  • 3. Substituting equation (2) in (1) Equation (3) is From Maxwell’s Equation
  • 5. Integrating throughout the volume Total Power Power Rate of energy stored dissipation Using divergence theorem
  • 6. Power flow in a co-axial cable Consider a co-axial cable which has a dc voltage ‘V’ between the conductors and a steady current I flowing in the inner and outer conductors. The radius of inner and outer conductor are ‘a’ and ‘b’ respectively. + b a I V Resistance -
  • 7. By ampere’s Law: Circumference of circular path between a and b =2πr
  • 8. E due to an infinitely long conductor Equation (1) Where λ is the charge density. The potential difference between the conductors is Equation (2) E in terms of V from (1) and (2) is
  • 9. Power density Since E and H are always perpendicular to each other
  • 10. The total power will be given by the integration of power density P over any cross section surface. Let the elemental surface already be 2πrdr Total power
  • 11. i.e. The power flow along the cable is the product of V and I