Module 2 : Transmission Lines
Lecture 6 : Loss Less Transmission Line
  Analysis of Loss Less Transmission Line
In any electrical circuit the power loss is due to ohmic elements. A loss less transmission line therefore implies and . For a loss less transmission line hence we get
  Propagation constant :
 
  That is, and .
The charateristic impedance
 
The reflection coefficient at any point on the line is
 
The voltage and current expressions become
 
Let the reflection coefficient at the load end be written in the amplitude and phase form as
 
   then we have
 
   
As we move towards the generator the phase becomes more negative and point P rotates clockwise on the dotted circle. The radius of the circle is . Length of the vector OP gives the magnitude of the quantity