Two-Turn Inductor, One Turn Transformer

Derivation of Reflection and Transmission Coefficients

 

By Mike Gibson and Ivor Catt, June 1986

 

 

 

 

Here is a description of the symbols used in the derivations:

 

                VFC          voltage on cable moving towards the inductor

                VRC          voltage on cable moving away from the inductor

                ZC            characteristic impedance of the cable

 

                VFE          voltage traveling in the forward direction in the even mode

                VFO          voltage traveling in the forward direction in the odd mode

                VRE          voltage traveling in the reverse direction in the even mode

                VRO          voltage traveling in the reverse direction in the odd mode

                ZE            characteristic impedance of even mode

                ZO            characteristic impedance of odd mode

 

                VFS          secondary voltage moving away from the transformer

                VRS          secondary voltage moving towards the transformer

 


 

From the Cable into the Inductor

Going from the cable to the inductor, the following basic equations hold,

 

                1)            

                2)            

                3)            

 

Transforming (2) into voltages gives,

 

                4)            

 

Multiplying through by ZC and defining new terms for the resulting ratios yields,

 

                5)            

 

                6)                        

 

From (1),

 

7)            

 

Substituting (7) into (5) and gathering terms,

 

                               

                8)            

 

From (3), VFO = VFE . Substituting this into (8) gives,

 

                               

 

 

                8)            

 

                9)            

 

Substituting VFE and VFO from (8) and (9) into (7) gives the reflection coefficient,

 

                               

 

 

                10)          

 

 


 

From the Inductor into the Cable

Going from the even and odd modes in the inductor to the cable, the following equations hold,

 

                1)            

                2)            

                3)            

 

Reflection coefficients can be derived using the same procedure as in the Cable to Inductor section,

 

                4)            

 

                5)            

 

                6)            

 

                7)            

 

Using these, the transmission coefficients to the cable can be derived,

 

                8)            

 

                9)            

 

 


 

From the Transformer into the Secondary

Going from the even and odd modes in the transformer to the secondary cable, the following equations hold,

 

                1)            

                2)            

                3)            

 

Two new ratios emerge in the derivation of the reflection and transmission coefficients,

 

                4)                       

 

The resulting reflection coefficients are,

 

                5)            

 

                6)            

 

                7)            

 

                8)            

 

And the resulting transmission coefficients are,

 

                9)            

 

                10)          

 

 


 

From the Secondary into the Transformer

Going from the secondary into the transformer, the following equations hold,

 

                1)            

                2)            

                3)            

 

 

 

 

                1)            

 

                2)            

 

                3)